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In Conversation with Nima Arkani-Hamed

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In Conversation with Nima Arkani-Hamed

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0:16

My name is Yorus Kla. I'm a PhD student

0:19

here at the MPI MIS in in light.

0:22

>> And I'm Veronica. I'm also a PhD student

0:25

here. And also today we have Nema. And

0:28

could you maybe introduce yourself very

0:30

quickly?

0:30

>> Yeah, I'm Neimar Kani Hamemed. I'm a

0:33

theoretical physicist at the Institute

0:35

for Advanced Study in Princeton.

0:37

>> Okay. Good to have you, Nema.

0:40

Um so we would like to start out slowly

0:43

and all the way back from um and ask you

0:46

basically is there a particular reason

0:48

why you entered the field of physics or

0:50

science in general?

0:51

>> Yeah. Well, I mean I think uh um

0:55

probably like most people who end up in

0:57

uh in in in science. I I I loved uh

1:00

nature as a kid. Um uh actually I was

1:03

most uh fascinated by uh animals um for

1:07

a long time you know sort of natural

1:09

history. I wanted I would sort of catch

1:11

frogs and toads and snakes and things

1:12

like that and uh and attempt to study

1:15

them. Um and uh so I wanted to be a

1:18

naturalist for a long time but I'm the

1:20

child of two physicists and I'd like to

1:22

say it was my active teenage rebellion

1:24

to become a physicist. They definitely

1:26

did not want me to be a to be a

1:28

physicist. Um and uh uh also I loved

1:32

math from a from a from a young age. I

1:34

loved math and then I you know I put two

1:35

and two together that there was

1:37

something you could do with your life

1:38

that put these things about the natural

1:40

world and the world of mathematics

1:42

together. Actually I can say very

1:44

specifically the moment uh I decided I

1:46

was going to be a theoretical physicist.

1:48

Um

1:49

>> uh I think I was maybe 12 or 13 years

1:51

old. Um and um uh like most kids of that

1:57

uh era in the ' 80s, you know, I was

1:58

fascinated by the space shuttle going

2:00

going going up and down.

2:02

>> And I'd heard this number that you have

2:03

to sort of fire the rockets of the space

2:05

shuttle. So it goes at 11 km a second to

2:07

get out of the earth's uh gravitational

2:09

field. And you know, I wondered how do

2:11

they figure out that number 11 km a

2:13

second? Did they try 3 km a second?

2:15

Nope. Four? Nope. Five? Nope. You know

2:18

that. And at some point, woo, it goes at

2:20

11, right? some expensive

2:21

>> and uh yeah it sounds sounds expensive

2:23

and dangerous and my my uh my uh my my

2:28

father um explained to me uh really

2:31

basic things energy conservation

2:32

Newton's law I didn't know any of these

2:34

things but um but he just sort of

2:36

sketched out in a few lines uh the

2:38

formula v^2= 2gm over r for how you

2:41

could figure out escape velocity and

2:43

that just completely blew me away that

2:45

that you could figure that out and that

2:46

it was something a kid could understand

2:48

and a kid could do and now that I had

2:50

formula. I had the answer for the Earth.

2:51

I had it for Jupiter. I had for getting

2:53

out of solos. I had it for for

2:54

everything in one shot. And that just

2:57

kind of blew me away that there was a

3:00

not only some sort of beauty and wonder

3:02

in the natural world, but some kind of

3:04

power as well in understanding it. Um

3:06

and that uh and that uh that really

3:09

hooked me and and around that time I I

3:11

really sort of decided fairly seriously

3:12

that I wanted to be a theoretical

3:14

physicist and uh and oriented my

3:18

life to start trying to to do that

3:20

>> and in all of this path since you were

3:23

12 years old until nowadays that uh I

3:26

mean it's a long time thinking about

3:27

physics of course do you have any

3:29

particular role model or role models

3:32

that were important? Oh, that's a great

3:34

question because I think um probably if

3:36

you ask most people I don't know if

3:39

people would have similar answers. Um uh

3:42

you know there's uh uh there's of course

3:46

uh heroes we have in all of uh all of

3:49

physics Newton Einstein Maxwell Dak

3:51

these people and um uh you know when I

3:55

was a kid growing up or or learning

3:56

physics there were these sort of gods

3:58

out there but I didn't think about them

3:59

too much other than thanking them. Thank

4:01

you Newton you know for uh for giving us

4:03

uh f equals ma but um I was sort of much

4:07

more fascinated as I said with the sort

4:09

of ability to use uh uh physics to to

4:13

explain things in the world around us.

4:15

uh you know along those lines um just as

4:17

a maybe a tangential comment in this

4:19

direction I was not personally

4:21

especially inspired by popular books

4:23

about physics they had they were almost

4:26

I I mean I wouldn't say uh explicitly

4:29

repulsive but definitely at most neutral

4:32

um uh because I could tell they were not

4:34

giving me the real deal you know that uh

4:36

and I was learning the real deal already

4:38

you know myself so I could figure out

4:40

where the rainbows were in the sky or

4:41

where you saw Mirage or you know uh

4:44

other things that that was possible to

4:46

figure out uh myself. Um so in that

4:49

sense the people who were the most

4:50

important to me uh early on were either

4:53

you know somewhat older kids who knew

4:56

things that could teach me um or you

4:58

know I had a few fantastic teachers um

5:01

uh I had an amazing uh physics teacher

5:04

when I was in uh grade 10. Uh his name

5:06

was John Wy um who had just gotten his

5:09

PhD um uh from the University of

5:12

Toronto. I grew up in Toronto in Canada

5:15

and um uh and you know could just tell

5:19

that I was crazy about physics and um

5:22

one of the most like amazing uh moments

5:24

of my intellectual life. Maybe one of

5:27

the most contentful sort of 90 seconds I

5:29

had was when he stared over my shoulder

5:31

and saw that I was, you know, working on

5:33

some complicated problem with incline

5:35

planes and balls and things like that,

5:36

which I sort of love to do. And he said,

5:38

"You know what? All these questions are

5:39

trivial. Um, you can solve them all in

5:43

one line with one method." I'm like,

5:45

"Get out of here. That's impossible. You

5:46

know, I'm I'm I'm I'm the world's expert

5:48

on complicated monkeys and pulleys and

5:50

fly planes. You know, you're telling me

5:52

there's a way of doing it any old schmo

5:54

can do." And he said, "Yes." and he

5:56

wrote down the lrangeian you know and he

5:58

did the whole thing in 90 seconds you

6:00

know he said you all you do is you write

6:01

down kinetic energy minus potential

6:03

energy then you write down this equation

6:04

he didn't derive anything he just wrote

6:06

down the oil lrange equation and as he

6:08

went said do you know what a partial

6:09

derivative is I said no he said just

6:11

pretend all the all the variables are

6:12

constant I'm like okay you know I can do

6:15

that I can do that and he went away and

6:18

then I'm like holy crap this can't

6:19

possibly work and I remember trying it

6:21

on the very first problem was not some

6:23

Mickey Mouse problem cuz I I I wanted to

6:26

see if this thing really worked. So I

6:27

did the problem of the, you know, mass

6:29

on a string spinning around attached to

6:32

a weight through the hole in the table.

6:33

I set it all up. I followed what he

6:35

said. I got the equations I knew you're

6:37

supposed to get

6:38

>> and it changed my life. You know that um

6:40

it really did change change my life

6:42

because I I appreciated not only is

6:44

physics amazing and you use it to

6:45

predict things in the world around you,

6:46

but there's structures underneath it.

6:48

There are some sort of deep structures

6:49

underneath it and that and that you're

6:52

not done when you get the first set like

6:54

F equals MA. you can sort of keep on

6:56

going, discover other things about that

6:57

that exploring the sort of structures

6:59

themselves is something uh meaningful.

7:01

Anyway, so here's an example. I mean, he

7:03

was incredibly important, not not like a

7:05

godlike role model per se, but those are

7:07

the most important people to me. It was

7:09

the people directly around me. You know,

7:10

when I was in graduate school, it was

7:12

like these slightly older graduate

7:13

students who sort of, you know, showed

7:15

me all the tricks tricks of the trade so

7:16

I wouldn't have to uh I wouldn't have to

7:18

flounder around. uh I think sort of much

7:21

later when I became uh you know not only

7:24

started doing research but you know

7:26

started having plans and sort of ideas

7:28

for what I wanted to spend years and

7:29

years of my life doing at that point we

7:31

could talk about uh the more

7:33

conventional sort of role model I guess

7:36

and there my answer is totally cliche um

7:39

but maybe uh hopefully not entirely

7:41

cliche reasons is probably Einstein um

7:44

and it's Einstein uh only because like

7:47

Newton and Maxwell are Martians uh sorry

7:50

and maybe not Maxwell I meant Newton

7:52

Durac uh people like that are clearly

7:55

have some sort of CPU and mental ability

7:57

that's uh not comparable uh certainly to

8:00

me or really most most most of people um

8:04

um uh you know Newton in in the

8:06

Principia would wake up in the morning

8:07

and decide he wanted to calculate square

8:08

root of two to 20 decimal places for fun

8:11

because he just discovered the binomial

8:12

expansion you know that's not that's not

8:15

uh that's not not me uh but uh I'm also

8:19

Einstein. Let me make that clear. Let me

8:21

make that very very clear. But um but

8:24

his his sort of the way he went about uh

8:27

doing physics and um uh was not driven

8:30

by some monstrous CPU. Of course, he had

8:32

an unworldly physical intuition, but he

8:34

made so many mistakes. You know, he made

8:36

so many elementary mistakes. He was

8:38

struggling for a long time. What he had

8:40

more than anything is some like

8:42

unbelievable

8:44

drive and will to stick with a hard

8:46

problem. ignore what everyone was

8:48

saying. No one believed him. No one

8:49

cared. Up, down. But somehow he had this

8:52

sort of drive to keep on going for years

8:54

and years and years until something made

8:55

sense. And uh that I find incredibly

8:58

inspiring. I mean that that's very very

9:00

difficult to do. But I've tried sort of

9:02

consciously very consciously in my life

9:04

to you know go longer and longer periods

9:07

without making progress uh before

9:09

getting freaked out and switching to

9:10

something else. and you know Einstein's

9:12

example you know other people uh you

9:14

know there's maybe more examples in in

9:17

in in math the wilds Pearlman people

9:19

like that um but it's this kind of uh

9:23

sticking to something with some

9:25

particular vision of what what might uh

9:28

uh what might happen um and uh

9:31

continuing until you get there has been

9:33

has been in some more concrete way uh

9:36

inspiring to me.

9:37

>> All right. All right. Okay. This is also

9:39

already good. you're moving a bit

9:41

further into your career already.

9:42

>> Okay.

9:43

>> So, and the followup on this would be so

9:46

one of the most prominent research

9:48

aspects that came out of your research

9:50

life um that interest us here lots is

9:53

the amplitude. Yes.

9:54

>> Is there is there like a bit of a story

9:57

how you came to think about it and how

9:59

it developed? How did you end up

10:00

defining it?

10:02

>> Oh yes. I mean it's uh um my work uh uh

10:06

even starting in uh graduate school and

10:09

through to about 2008 so about you know

10:12

15 years the first sort of 15 years of

10:14

my uh of my um uh I started grad school

10:18

in 93 okay so so that that period of my

10:22

life um I was not doing mathematical

10:25

things at all I mean I was uh most

10:27

interested in um uh in uh uh thinking

10:31

about theories for what we might see at

10:34

the large adon collider that sort of

10:36

attack problems of particle physics.

10:37

There's a one of the great problems of

10:40

uh one of the great mysteries in nature

10:41

is we don't understand why the universe

10:43

is big. Um and that's because there's

10:46

sort of increasingly violent quantum

10:47

mechanical fluctuations at shorter and

10:49

shorter distances in the vacuum. What uh

10:51

seemingly create uh destroy any

10:53

possibility of of a macroscopic

10:55

universe. Uh and yet here we are. The

10:58

universe is very big. The universe has

10:59

large things in it. And uh those are

11:02

turn out to be huge mysteries we still

11:04

don't uh understand. If we take for

11:06

granted that the universe is big and

11:08

that it has big things in it. This is

11:10

tantamount to the existence of very

11:12

large sort of hierarchies of scale

11:13

between very microscopic length scale

11:16

like the like the plunk scale where

11:17

where where gravity gets strong spaceime

11:19

breaks down etc etc. And the much larger

11:23

scales in the universe all the way out

11:24

to the size of the observable universe

11:26

sort of six orders of magnitude between

11:28

the plunk length and the size of the

11:29

universe. and many other scales that

11:31

populate things in between that are very

11:33

well separated from each other. And the

11:35

big mystery is why quantum fluctuations

11:37

don't sort of crash all those scales on

11:39

top of each other. So it's not an

11:40

esoteric question. It's some very basic

11:42

question about the world around us. Um

11:45

uh you know when when I was in

11:47

undergraduate uh I mentioned even as a

11:50

kid I loved math and I loved physics. I

11:52

love both of them. I just all love

11:53

physics always very slightly more very

11:56

very slightly more but it was a very

11:58

slight thing. It was very difficult for

11:59

me to sort of choose definitely to be a

12:02

theoretical physicist and not a not a a

12:04

mathematician. But that choice kind of

12:06

affected a lot uh uh what I did because

12:10

I always had in back of my mind if I was

12:12

going to do something more mathematical

12:13

and formal uh I wasn't going to do

12:15

something sort of half-ass, I might as

12:17

well be a mathematician if I'm going to

12:18

do that, not you know. Um so so you know

12:21

I polarized more into questions that

12:24

would have uh uh direct contact with

12:26

experiment and that's that's really what

12:28

what I what I focused on and what I

12:30

worked on. Anyway, there's many twists

12:32

and turns in this story, but um uh but

12:37

uh in the mid 2000s uh me and many other

12:40

people uh started becoming alive to a

12:44

very different possibility for what

12:46

might explain uh these mysteries like uh

12:48

why the universe is big, why it has big

12:50

things in it. um uh related to ideas of

12:54

uh uh the possibility that uh uh the

12:57

constants of nature, what we think of as

12:58

a constants of nature. And these

13:00

mysteries about the vastness of the

13:01

universe are related to some of the

13:02

constants of nature like uh the vacuum

13:05

energy, the cosmological constant uh

13:07

it's called the cosmological constant or

13:09

uh the the the the constant that

13:10

controls the mass of the Higs particle.

13:12

Why these constants have seemingly

13:14

absurdly minuscule values compared to

13:16

what you would have sort of naturally

13:17

expected them to have.

13:18

>> So is this about naturalness? That's

13:20

right. This is this is the entire

13:21

question that uh that technically goes

13:23

by by by the name naturalness, but it's

13:25

really this sort of very basic question

13:26

about why quantum fluctuations don't

13:28

wipe out uh uh microscopic order and uh

13:32

and a sort of possibility started

13:34

emerging that maybe the constants uh are

13:37

not actually constant and they they they

13:38

they take on different values in

13:40

different regions of uh not the

13:42

observable universe, but if you're

13:43

somehow in a god's eye picture, zoom out

13:45

to gargantuan scales, you would see that

13:48

there is a giant multiverse out there

13:50

and the constants take different values

13:51

in different places in the universe and

13:53

in most of those places um if you change

13:56

these constants a little bit the

13:57

universe is empty or doesn't have any

13:59

matter of any sort in it or any

14:01

structure in it uh uh and so um it's

14:04

lethal mostly out there but in a few

14:06

tiny spots of uh it's possible for

14:09

structure and life to emerge and that's

14:10

why we we find ourselves there anyway it

14:13

was a sort of a controversial idea it's

14:15

still a controversial idea uh but people

14:17

tried to make sort of more proper for

14:19

theoretical sense of it. They tried and

14:22

they failed and uh they uh and I tried

14:24

and I failed. Many people tried and

14:26

failed. Um but these questions sort of

14:29

convinced me that uh we did need to

14:32

learn even for questions of direct

14:33

relevance to experiment you know not uh

14:36

you know questions up at the the the

14:38

scale having to do with quantum gravity

14:39

and so on that one way or another we

14:41

needed to figure out how to make sense

14:43

of quantum mechanics and cosmology uh

14:46

all in the same sentence. Right? that um

14:49

uh that that we couldn't factoriize

14:51

these sort of deep conceptual questions

14:53

about quantum mechanics in in the

14:54

universe from the more practical seeming

14:56

questions of the sort of structure of

14:58

our vacuum. And uh that's a very hard

15:01

question. But when you start backing up

15:03

from that question, at least I found

15:05

myself running into a simpler version of

15:08

all these problems where you try to uh

15:10

it was clear you somehow have to

15:11

reconceptualize what quantum mechanics,

15:13

spacetime, and the vacuum are about.

15:14

That's sort of that's I think completely

15:16

clear that continues to be clear today.

15:18

Uh but um uh but trying to do that in

15:21

the directly in the context of these

15:22

cosmological questions seemed too

15:24

difficult. And so I sort of tried to

15:26

back up to the first setting in which it

15:28

seemed like you could do something about

15:29

it. Um and uh so time has to be

15:32

important just like it's important in

15:34

cosmology. Dynamics has to be important.

15:36

You have to think about some questions

15:38

where quantum mechanics and spaceime

15:39

matter at order 100% you know in some

15:42

vivid way. And so uh scattering of

15:45

elementary particles was the sort of

15:46

obvious uh uh version of that uh

15:50

question. I had also learned um first

15:53

through the sort of famous paper of

15:54

Edward Whitten in 2003 um you know with

15:58

some vision for what an alternate theory

16:00

of scattering amplitudes might be. I was

16:02

not working on the subject at all but I

16:04

knew this seemed like a big deal. And

16:06

secondly, through the work of some

16:08

brilliant young people who also later

16:09

collaborated with Edward about these

16:11

things, including uh Freddy Kachazo uh

16:14

and Ruth Bridto who's uh uh here who

16:17

were both students at uh Harvard uh when

16:19

I was when I was there. I knew that

16:21

something was a foot in this world of of

16:23

amplitudes that there were you know very

16:25

basic facts about quantum field theory

16:27

that uh were being understood in new

16:29

ways. Um and uh that I found very very

16:33

striking. You know, I I thought of

16:35

myself as someone who maybe didn't know

16:36

all the fancy esoterica of uh what was

16:39

going on in uh field theory, but I I

16:41

understood the basics. I thought cold,

16:43

right? And then, you know, I remember

16:45

Freddy telling me some amazing things uh

16:47

that uh were associated with the famous

16:49

BCFW recursion relations, but they

16:52

involved some simple properties of uh

16:55

amplitudes that I just simply didn't

16:56

know. And of course, nobody knew before

16:58

they discovered them. So that that I

17:00

found uh very striking that there was

17:03

something going on uh right under our

17:05

noses that that we didn't understand.

17:07

And anyway, so those were all the

17:09

motivations in uh something like 2007208

17:13

to uh stop what I was doing and and

17:16

start uh uh start thinking about uh

17:18

amplitudes. The the the year or two uh

17:21

leading up to this period I was uh it

17:23

was also uh in anticipation of the Large

17:25

Hadron Collider turning on. So I'd spent

17:27

a lot of time thinking about uh you know

17:29

very practical questions about better

17:31

ways experimentalists might look at the

17:32

data coming out of the LHC. So that's

17:34

why maybe as I said in the beginning of

17:36

the child lectures the period before

17:38

amplitude is I was mostly working with

17:40

experimental particle physicists. Uh but

17:42

um variety of reasons there was kind of

17:45

a hard stop uh um I moved to the

17:48

institute for advanced study and that

17:49

was also a great opportunity to just

17:50

sort of become a graduate student again

17:52

for a while and learn a new subject. uh

17:54

and so um yeah so that's when it started

17:57

in uh uh 2008 um but it started with

18:00

this very clear picture uh I mean I

18:04

would go to conferences and say this is

18:06

what uh I I wanted to happen you know

18:08

some some people were friendly some

18:09

people were skeptical but it was a very

18:11

clear picture that what we're looking

18:12

for is some new way of formulating what

18:15

scattering amplitudes are where we

18:16

didn't have the usual apparatus we

18:18

didn't have uh uh we weren't relying on

18:21

pictures of particle trajectories or the

18:23

evolution of the wave function in in

18:25

Hilbert's space. Um, of course, this was

18:28

not coming entirely out of the blue. We

18:29

had this sort of stunning success of

18:31

BCFW recursion was clearly organizing or

18:34

thinking in some radically different

18:35

way. Even though you could, of course,

18:37

derive it in principle. There's a

18:39

derivation from standard quantum field

18:40

theory. So, you could, if you're a

18:42

skeptic, say, okay, it's very cool. It's

18:44

a tool. It's a tool, right? It's a it's

18:45

a very cool tool. You can derive it from

18:47

field theory and so on. But it also

18:49

looked like it was organizing things in

18:51

such a radically different way that that

18:53

you you had to be able to interpret them

18:54

as coming from a different world of uh

18:56

ideas. And so that that was it. It was

19:00

really kind of a a five-year period

19:02

between 2008 and 2013 that kind of saw

19:05

this uh evolution towards ampl happen in

19:08

steps. Um uh I spent uh a year with

19:12

Freddy Kachazo visiting me at the

19:13

institute. I like to tell Freddy that I

19:16

was uh I mean I was his grad student for

19:18

that year. I told him for a while, you

19:20

know, I would be his best grad student

19:21

ever, but he's had really good grad

19:23

students since, so it might not be true

19:24

that um and uh but I learned an enormous

19:28

amount from him in that year and we

19:30

started doing uh some work together that

19:32

uh started thinking about what these

19:34

recursion relations like BCFW meant in

19:36

twister space. That was the sort of

19:38

first first step. And then that led us

19:41

to uh uh sort of drawing pictures for

19:44

how we thought about these things in a

19:45

twister space that looked eerily similar

19:48

to pictures that one of my uh real

19:50

heroes in uh all of physics uh um uh

19:54

really heroes in life uh uh Andrew

19:56

Hodgeges at Oxford um had been drawing

19:59

uh since he was Penrose student in the

20:01

70s. Okay. Um, and I'd been staring at

20:04

Andrew's papers that been sitting on my

20:06

desk for two years. For these two years,

20:08

I couldn't figure out if he was a, you

20:09

know, crackpot or a genius. Uh, and, uh,

20:12

it was it was the latter, you know,

20:14

that, but but it took two years to, uh,

20:16

to figure that out. And, uh, Freddy and

20:18

and I and and and, uh, and and and some

20:22

of my, uh, uh, students back then

20:24

started figuring out the pictures that

20:25

we're drawing looked a lot like, uh,

20:27

Andrew's pictures. And we spent a number

20:29

of weeks with our crappy pictures on the

20:32

board on one side and his beautiful

20:34

pictures on the other side and and

20:35

asking what would we have to do to our

20:37

pictures to make them look more like

20:38

Andrew's pictures and along the way

20:40

discovering all sorts of uh wonderful

20:42

things. Um uh that ended up connecting

20:46

to the to Grassmanians in some way. So

20:48

that so understanding those pictures

20:50

ended up connecting to Gusmanians. That

20:53

was a whole other fantastic set of uh

20:56

coincidences that Alex Posnikov had

20:59

worked out essentially what the

21:00

structure uh looked like just a little

21:02

while before we needed it. But we ran

21:04

into uh uh Sasha Garcro is incredibly

21:08

important in in having us think about

21:10

these things properly. We spent months

21:12

um uh interacting before we knew any of

21:14

these things with Pierre Delene uh at

21:16

the institute who uh uh you know was

21:18

another you know heroes is uh I mean

21:22

he's one of these people it's hard to be

21:23

a hero because he's on a different plane

21:25

but um but still incredibly important

21:27

sort of getting us in the oriented and

21:30

and thinking about things the right way

21:32

and so that was a sort of penultimate

21:34

step. So, so we figured out how all the

21:36

building blocks for amplitudes um were

21:39

were were or organized according to

21:41

concepts in the Gmanian and the positive

21:42

Gmanian and so on. And that was a sort

21:45

of uh so that was that then the the

21:47

final step was to sever all ties to

21:50

standard uh notions of uh field theory.

21:53

So everything up to that point, you

21:55

could if you wanted to still connect

21:57

everything back back back to some

21:59

relatively conventional uh uh ideas in

22:03

uh in field theory. And so there was

22:05

like a last period of a year and a half

22:07

or two years where uh where we we

22:10

struggled a lot to see where all of

22:12

these pieces all the ways of building

22:14

amplitudes by putting together pieces.

22:16

Uh the pieces could be thought of as in

22:18

terms of BCFW or they be thought of in

22:20

terms of onshell processes or they could

22:23

be thought of in terms of uh uh uh

22:25

building blocks in the positive grasman

22:27

but they're all still kind of Lego

22:29

blocks that were being assembled in some

22:31

way but we didn't know what they were

22:32

assembling into. And uh so that was

22:35

maybe the most everything up to the

22:37

point I was describing was a joy ride

22:39

because everything just worked more or

22:40

less out of the box. It just worked. uh

22:43

you just have to sort of head in the

22:44

right direction and it just uh it was

22:46

like uh uh walking through an open door

22:49

almost. Um the last period was much more

22:52

more difficult because uh somehow two or

22:54

three ideas had to exist in your head

22:57

simultaneously in order to see the right

22:59

thing to do next and it took us a couple

23:00

years to uh to see it. But even then it

23:03

was not totally hopeless because so many

23:06

little miracles had happened that we

23:07

just knew the thing that we're looking

23:09

for had to exist that um and there were

23:12

sort of uh experimental uh there you

23:15

know miraculous identities that the

23:17

amplitude satisfied lots of little

23:18

numerical experiments that made it clear

23:20

that the kind of object we're looking

23:22

for had to exist. So so there's a reason

23:24

not to give up even though uh it wasn't

23:26

clear uh what it was. Anyway, so that's

23:28

the uh that's the story. It was about a

23:30

sort of a 5-year period. um uh from 2008

23:33

where it all started to uh 2013 when we

23:36

ran into the object. Then yeah maybe

23:38

fast forward in then 10 years from 2013

23:41

to let's say 2023 2024

23:45

uh sort of the the this ERC grant among

23:48

which these cow lecturers make part of

23:51

the universe plus grant

23:52

>> came to be

23:54

>> and we wanted to ask you in your eyes

23:56

what is the most exciting aspect that

23:58

has came out

24:00

>> um of this universe plus grant so far?

24:02

Well, I mean, I think uh I think it's uh

24:05

to start with, I'd say it's mere

24:06

existence is exciting. Um uh I mean it

24:10

it exists because of a large number of

24:13

uh of kind of scientific things that

24:15

have happened over the past uh 10 10

24:18

years. Um uh I think that the for me

24:22

personally that that the story of of the

24:23

of the amplahedron was uh was sort of

24:26

crucial for seeing that that some vision

24:29

of this sort for what the laws of

24:30

physics might look like is possible.

24:33

Right? But of course uh it was for very

24:35

limited set of theories uh in very

24:38

special cases and so on. Um you could

24:41

say as many dimminitive things about it

24:42

as as you wanted and I would agree you

24:44

know. So, so, so, um, uh, so the goal

24:49

was try to always to get closer and

24:50

closer to describing, uh, reality. Um,

24:54

uh, my my attitude about this as a

24:57

physicist is that as we get closer to

24:59

the real world, we should expect to see

25:01

more magical structures, not less. uh

25:03

and uh that maybe contrasts a little bit

25:06

with the attitude of some more

25:07

mathematically minded physicists who uh

25:10

say well you know you see exciting

25:12

mathematical structures and toy models

25:14

that have some properties they're

25:15

integraable they have this they have

25:17

that but uh but it's sort of cool things

25:19

about mathematical physics it's unlikely

25:21

you're going to see something like that

25:22

in the real world. My attitude is the

25:24

opposite. You know the closer we get to

25:25

the real world it has to get there's

25:27

nothing more magical than than than the

25:29

real world. So, it's very unlikely. If

25:31

you believe uh uh in this deep

25:33

connection between the the Platonic

25:35

mathematical universe and and and and

25:37

the real world, which I certainly do, uh

25:39

then it's just impossible to believe

25:41

that if there's something magical in the

25:43

little corner that there isn't something

25:44

vastly more magical uh actually going on

25:47

in in in in the real world. So, that

25:50

that was a belief, but it was only a

25:51

belief. And uh you know in various steps

25:54

uh we started uh seeing things uh uh

25:57

with the kind of character of the story

25:59

of the amplean but but quite different

26:01

in in um in uh in technical realization

26:06

uh emerge in the period after 2013. At

26:09

the same time um uh so so first even

26:12

purely within physics similar ideas

26:14

started emerging in in in cosmology. So

26:17

um and uh that uh that should

26:22

surprise you that that you know we're

26:24

we're it should it should seem at least

26:27

on the face of it surprising there's any

26:28

commonality between scattering

26:30

elementary particles and lying your back

26:32

and looking at the night sky and sort of

26:34

correlating what's happening here and

26:35

there and there don't on the face of it

26:37

seem to be similar problems. Of course,

26:40

technically they're they're very closely

26:41

related that they're they're both

26:43

computed in the same kind of uh you

26:45

know, quantum field theory formalism um

26:48

uh and in a it turns out in a very

26:50

precise sense that these sort of

26:52

correlations you observe in the sky and

26:53

cosmology swallow and contain the

26:56

formulas that give you uh scattering for

26:59

uh uh uh elementary particles. Um so

27:03

they end up being more closely related

27:05

than than than you might think. But

27:06

anyway, similar kinds of pictures,

27:08

similar sort of combinatorial geometric

27:10

pictures for what might be explaining um

27:13

uh uh cosmological correlations started

27:16

emerging in this intermediate period.

27:18

And finally um this is when uh it sort

27:21

of happened that my dominant

27:23

collaborators went from being

27:24

experimental theoretical physicists

27:26

experimental physicists theoretical

27:27

physicists to being mathematicians. And

27:29

um and that really blew me away. I mean

27:32

you know that um they're amazing group

27:33

of people uh brilliant um of course

27:37

think about things in totally different

27:38

ways than uh I do um and uh the most

27:42

fascinating thing to me was that um uh

27:46

uh we are not in one of these typical

27:48

situations either where the

27:49

mathematicians had figured everything

27:50

out already and then the physicists came

27:52

to use it as a tool which is maybe the

27:54

most common way this interaction looks

27:56

like or the the sort of interaction

27:59

where you know physicists know quantum

28:00

field theory string theory can predict

28:02

all sorts of things and mathematicians

28:04

have to come and figure out how to prove

28:05

it later where um uh well maybe

28:08

mathematicians care about the proving it

28:09

part but if you're a physicist you're

28:11

like I'd rather know how to make the the

28:12

the correct statements um but this is

28:15

not either one of those it's a it's a

28:17

bizarre situation where time and time

28:19

again um I mean I mentioned the story of

28:21

Pasikov and the positive Rasmanian right

28:23

when we needed it not 50 years before

28:25

you know like a few years before uh but

28:27

it just keeps happening over and over

28:29

again it's like we're running into the

28:30

same beast from different directions.

28:33

It's utterly bizarre that it's happening

28:34

roughly uh you know simultaneously. Um

28:38

and it means that when we talk to each

28:39

other, it's useful. You know, it's not

28:41

just uh interdisciplinary conversations

28:44

because it's cool to be

28:45

interdicciplinary. Far far from it. You

28:47

know, we're being sort of we're

28:49

individually experts in what we do, but

28:51

we're being dragged into some common

28:52

boundary because we're seeing the same

28:54

thing. Um and uh it's been incredibly

28:57

exciting working with like a large

28:59

number of different uh uh groups of uh

29:02

mathematicians. So um the answer to your

29:05

question I think just the the the

29:07

existence of the of this uh of this uh

29:10

of this project that's that's supposed

29:12

to bring together cosmology, particle

29:14

physics, mathematics in this uh you know

29:18

in this joint area where something

29:19

clearly is is happening um I think is

29:22

remarkable. You know, if you told a a

29:24

collider physicist 15 years ago that

29:26

grossmanians and cluster algebbras and

29:29

you know total positivity of matrices

29:31

with all positive determinants had

29:33

anything to do with anything, they would

29:34

think you're insane. You know that this

29:36

is not one of those, you know, it's not

29:38

one of those, you know, things between

29:39

math and physics where you kind of see,

29:41

yeah, probably they'll be related. It's

29:42

just insane that these things are

29:44

related. And if you told the

29:45

cominatorialists that what they're doing

29:47

playing around with like pictures of uh

29:49

permutations had anything to do with

29:51

what's going on when you collide

29:53

particles out there in nature or

29:54

accelerators or whatever, they would

29:55

also think you're you're insane. So um

29:57

so the fact that it's true is is

29:59

remarkable. And so I think the it's it's

30:01

it's just exciting uh to have more

30:04

systematic uh attitude about it. Having

30:07

said that, there are a couple of

30:09

specific things really specific sort of

30:11

dreams that that uh that at least I've

30:14

had that you know we even you dutifully

30:17

put in these proposals. We we are going

30:19

to do XYZW

30:21

which uh of course you know you have to

30:23

put something in a proposal but but when

30:24

you when you're doing research you go

30:26

wherever the hell the research takes you

30:27

but

30:28

>> but uh but a couple of the things just

30:30

hap just you know happened um uh much

30:34

earlier than I uh than I expected. Um,

30:37

one of the things that I've been looking

30:38

to do since 2017 is find a more I I I'd

30:43

mentioned back in 2017, we'd found some

30:45

very simple toy example of one of these

30:47

geometries that might be relevant for

30:50

cosmology, but we did not have a sort of

30:52

a complete picture of a geometry that

30:54

might be, you know, that might sort of

30:56

capture all possible processes uh

30:58

contributing to a uh to a cosmological

31:01

observable. um uh even in a toy model.

31:06

And um and uh we ran into that object

31:09

back in December. So that was something

31:11

I mean I I had no idea how long it would

31:13

take to find it, but I certainly tried

31:14

for many years and failed. Uh and we via

31:18

a few happy accidents uh ran into it in

31:20

December. before that um something else

31:23

you know we're talking about in the

31:25

proposal uh which I equally thought

31:28

would take years and years uh uh to find

31:30

but happened very suddenly and very very

31:33

quickly is some sort of version some

31:35

friend some cousin of the empahedron uh

31:38

to to describe directly the sort of

31:41

gluons the particles and the strong

31:43

interactions in in the real world not in

31:45

toy toy models and um there were a

31:48

number of ideas that had been developing

31:50

with collaborators over the course of

31:51

the pandemic uh um that uh that had a

31:54

sort of another approach to thinking

31:56

about all of these questions involving a

31:58

different set related but rather

32:00

different set of uh mathematical and and

32:02

physical ideas. Um but again there were

32:04

very toy theories and I thought okay

32:06

after we get the toy theory settled

32:08

we'll start again you know have to more

32:10

work uh and uh it was again like uh

32:14

going through an open door. It turned

32:15

out to be much closer uh in a surprising

32:18

way much much closer to sort of connect

32:20

these uh uh these toy theories to really

32:22

realistic theories that uh that describe

32:26

actual parts of the real world than I

32:28

thought. So those are two things I'm

32:29

extremely excited about. I did not

32:31

expect to happen as quickly as they did.

32:33

Um, but uh there are several more things

32:35

that we promised. Uh, we'd like to

32:38

figure out I mean really our goal is to

32:40

try to describe all of nature from this

32:42

point of view. We're very far from doing

32:44

that. Uh, but uh, we're working on it.

32:48

>> All right. I think just building on on

32:51

that um, do you think beyond what you

32:54

just mentioned which tied some toy

32:56

models closer to theories of nature? Is

32:59

there something re um other than that

33:01

example you gave which um in recent

33:03

developments got you excited of pushing

33:06

further and further into the theories of

33:08

nature? Uh yeah, I mean uh there are

33:12

clues lying around for uh what might uh

33:15

uh what might push us further in that

33:17

direction. I would say that maybe the um

33:21

uh

33:24

the main

33:26

qualitative large open problem um is uh

33:30

how so uh so far the so that this this

33:33

point of view um is uh starts with very

33:37

primitive questions right you know so

33:39

the the for example if you're talking

33:40

about uh a scattering of uh elementary

33:43

particles what we're doing is we throw

33:45

some particles in from far away uh

33:48

they're they're moving uh in some

33:49

directions. They have some energy. They

33:51

have some momentum. So you specify the

33:54

uh you specify their momenta that tells

33:56

you Einstein tells you their energy. Um

33:59

so bunch of momenta you know little

34:01

threedimensional vectors saying the the

34:03

directions they're coming in abracadabra

34:05

something happens and then a bunch of

34:07

things are going out. So that's the data

34:10

of the problem you know. So um uh you

34:13

get a function literally a function it

34:15

depends on these three vectors the these

34:17

three vectors that specify the uh uh uh

34:19

the particles going in and the particles

34:22

going out. Um and the kind of normal

34:25

apparatus of physics a normal way we

34:27

think about these things is by thinking

34:29

about the trajectories of particles

34:31

moving in space and time interacting and

34:33

that of course has all of the all of

34:36

physics in it. Right? So particles are

34:38

moving in space and time to get close to

34:40

each other. So there's a notion of

34:41

distance and they get close to each

34:42

other. When they hit each other, there's

34:44

an interaction. Uh uh then they then

34:47

they they produce something else. They

34:49

decay and so on. So there's a there's a

34:51

sort of whole picture that involves all

34:53

the apparatus of uh of uh uh of of

34:56

modern physics to figure out what what

34:58

what the answer is. But you see all of

35:00

that apparatus lives kind of on the

35:03

inside of this uh uh scattering process

35:06

in the in the inside of the space time

35:08

and these particles are thought to be

35:09

moving and so on. The actual question is

35:13

not posed on the inside of the of the of

35:16

this uh uh region of space and time.

35:19

It's just a question about a bunch of

35:20

vectors going in and a bunch of vectors

35:22

going out. So that's the canvas. The

35:24

canvas in which we're trying to build a

35:26

mathematical universe. Uh an alternate

35:29

picture for what could be describing

35:31

this process. The canvas is just you

35:34

know you have seven particles involving

35:36

the scattering process. Seven

35:37

threedimensional vectors. That's that's

35:39

that's the space. So you have to figure

35:41

out what to do in this world of like a

35:42

bunch of uh vectors. Uh and it seems

35:45

like an empty and austere world where

35:47

there isn't much to do. Um but it turns

35:50

out with a very very few uh extra

35:53

assumptions there's just enough

35:55

structure in these spaces where

35:57

something kind of magical can happen.

35:59

But one of the most important uh uh

36:02

elements uh that has allowed this to

36:04

happen in the mathematics is that you

36:07

imagine that these these vectors are not

36:09

just uh handed to you sort of randomly.

36:11

Here are seven vectors but they're rand

36:13

they're handed to you in some order.

36:15

Here's vector for particle one then

36:17

particle two particle three particle

36:19

four and so on. It seems like a

36:21

completely innocuous tiny thing but but

36:23

being handed in a particular order is

36:26

turns out in physics to be closely

36:27

related to the particles having uh what

36:30

we call color. So in the the the

36:33

strong interactions uh uh the particles

36:36

can be thought of as as having colors

36:38

and the way the colors flow from one

36:41

particle to the next is responsible for

36:43

this ordering. Um so all of the progress

36:47

at least all the progress that uh that

36:49

that this line of thinking that I've

36:51

been involved with um uh uh has been

36:56

centered around involves uh thinking

36:58

about particles with color. Now a lot of

36:59

particles in nature have color. Uh the

37:02

strong interactions there's a notion of

37:03

color. The weak interactions is a notion

37:05

of color. This notion of color is

37:07

ubiquitous. But some of the most

37:09

important things don't have color. You

37:10

know there's no notion of color

37:11

associated with photons. there's no

37:13

notion of color associated with gravity.

37:15

And so trying to understand how we have

37:18

a picture like this when you don't have

37:20

color and you don't have a notion of

37:22

sort of ordering um is a very deep and

37:24

basic one, you know. So um because it

37:26

seemed like it was the lifeline that let

37:28

something happen out of seemingly

37:30

nothing. And so we really have to go

37:32

back and and and and ask if there does

37:34

not seem to be anything, if there is no

37:36

no color, what could be the organizing

37:38

principle that lets us uh know what to

37:40

do next? that I think is the sort of

37:42

largest open problem. Um that's one I

37:46

mean we can we can we can say we'll

37:48

study it. We can say that we'll we'll

37:49

work on it. I've studied and worked on

37:51

it off and on for uh you know uh 10

37:54

years. Uh you never know what kind of uh

37:57

what uh set of accidents you'll uh uh

38:00

and uh happy coincidences will happen

38:02

along the way that might that might give

38:04

the key for where to go next. But there

38:06

is in this uh in this in this new set of

38:09

ideas um there is like a clue that uh

38:13

that that uh that at least at the level

38:17

of combinotaurics

38:18

um uh the world of gravity of uncolored

38:21

particles is sort of sitting there in

38:23

the structures that we're talking about.

38:24

That's very encouraging. So it's not uh

38:27

not only is it not absent, it's sort of

38:29

very much present. It's very much

38:31

present but in a very confusing way

38:32

right now in a way that we don't know

38:34

how to sort of turn into formulas that

38:37

physicists care about you know formulas

38:38

for scattering processes but they are

38:41

sitting there and so that's why I sort

38:42

of feel if we trump around in this

38:44

neighborhood for a while we might find

38:46

the right clue uh to let us make

38:48

progress but I think that's the sort of

38:50

biggest the most exciting question um uh

38:53

the biggest sort of potential obstacle

38:56

to the whole program and but one where

38:59

there's uh some possible clue for making

39:01

progress.

39:03

>> Sort of tying in also to something you

39:05

mentioned, I mean you've mentioned all

39:07

along the interview, you have definitely

39:09

been a key figure in pushing

39:11

interdisciplinary research between

39:13

mathematics and theoretical physics. Why

39:16

do you think this is important and how

39:19

could we make physicists and

39:21

mathematicians engage even more with

39:23

each other?

39:25

Well, um I I uh

39:28

I have a kind of maybe a funny attitude

39:30

towards interdisciplinarity which I've

39:32

maybe mentioned before. Um uh I've

39:36

always been personally suspicious of

39:38

interdicciplinary work. Um um uh I sort

39:42

of prefer to think of it as

39:43

cross-disciplinary than inter uh

39:46

interdisciplinary by which I mean um I'm

39:49

I'm suspicious. I mean I'm not I'm not

39:51

saying like actively hostile. I just I

39:53

literally mean

39:55

suspicious because I know many examples

39:57

of people who are sort of professional

39:59

interdisciplinarians which they mean

40:01

they permanently live at a boundary

40:02

between two fields

40:04

>> and um and then in almost all examples I

40:07

know when you like you know the fields A

40:09

and B uh when you ask people in field B

40:12

what they think of the work of this

40:13

person they say oh they're an expert in

40:15

A and when you ask the other way around

40:17

they say they're they're an expert in B.

40:18

I don't like that so much you know that

40:20

um uh I prefer cross-disciplinary

40:23

because it means uh it means that there

40:25

is someone who is you know science is

40:28

hard right you know we specialize for

40:30

good reasons um but um the the bad thing

40:33

about uh the worst thing about

40:36

specialization is not that you have to

40:37

sort of uh drill deep and know you know

40:40

one thing in order to make progress

40:43

that's all true that's life I mean you

40:45

know that's where where where we are in

40:46

the 21st century with our uh with the

40:48

way science works is if you do that so

40:51

much that you be sort of become blinded

40:52

to uh other things uh that are going on

40:55

elsewhere. You don't even sort of hear

40:56

about them. They don't sort of enter

40:58

your your your mind. Um and um uh but it

41:03

can happen, it does happen that the

41:05

exigencies of your own little thing that

41:07

you're working on, you know, force you

41:08

to a boundary, right? Um and it's even

41:11

more exciting when they force other

41:12

people on uh to the same boundary and

41:14

and you don't quite know why, but

41:16

something has dragged you there. uh

41:18

together. That's definitely been the

41:20

sense of this subject. That's why I

41:21

mentioned before, you know, it's not 15

41:23

years ago, it would have been insane to

41:25

think that that the cominatorics and

41:26

particle physics and geo have anything

41:28

to do with each other, but people were

41:30

dragged there uh together. Um once that

41:33

happens, I think it's extremely exciting

41:34

because because you're not just there

41:36

for the sake of being interdisiplinary,

41:38

you were dragged there for a reason and

41:40

you want to talk to each other because

41:41

they know something that that you need

41:42

and maybe vice vice versa. Um so um uh

41:47

uh I have to say my my interactions with

41:50

mathematicians have had none of the uh

41:53

sort of stereotypical flavor that you

41:55

sometimes hear interaction between

41:57

mathematicians and physicists have. Um

41:59

it has not been it has not remotely

42:02

revolved around the access of like you

42:04

know a physicist uh uh uh on the

42:08

frontier not caring at all about rigor

42:11

and the mathematicians caring about

42:13

rigor and dotting all the eyes and

42:14

crossing all the tees. Not remotely. I

42:16

mean it's not like that at all. Um of

42:19

course they care about rigor and proving

42:20

things more than we do. But it's a

42:22

sideshow that uh um much more

42:25

interestingly there's kind of a creative

42:26

tension between um trying to make

42:29

definitions and uh precise uh versus

42:32

not. I mean um uh as a physicist I'm

42:35

always a little nervous about making

42:37

definitions precise because I always

42:38

worry that we're trying to make things

42:40

precise too early uh and that if we just

42:43

wait a little bit longer we'll see what

42:44

the sort of correct structure is that we

42:46

should be talking about. So I don't want

42:47

to commit too early. Um uh and uh as a

42:51

physicist I also had the prejudice that

42:53

I was right you know uh but I've learned

42:55

on a number of occasions that my friends

42:57

on the other side were right that there

42:58

was sometimes this is a good time to

43:00

stop and try to say very be very precise

43:02

about what we're talking about um

43:05

because uh um once you do that and you

43:08

find something that works even in all

43:09

the degenerate cases then something

43:11

really good has happened. So that's

43:14

something that I have certainly learned

43:16

uh from uh uh interactions with my uh

43:19

mathematical friends. So even sort of

43:21

culturally that there was there are some

43:23

very useful parts in the way uh they are

43:26

thinking about things that uh that I've

43:27

definitely digested. I suspect that

43:30

they've picked up some things about the

43:31

way we go about doing things uh as well.

43:33

Um um but uh so it's been amazing. I

43:37

mean just uh and and and

43:40

not at all. Uh I've found sort of no

43:43

sort of cultural conflicts uh um even

43:46

the you know we don't understand each

43:48

other has been relatively minor. I mean

43:51

um of course that that they have a

43:53

different language uh and so on but

43:55

precisely because it's clear we're

43:56

seeing the same thing. Um it's uh it

43:58

doesn't take very long to say okay you

44:00

use these words we use this words but is

44:02

it about some matrix and does the matrix

44:04

look like this and do you do this thing

44:06

with it? It's like, yeah, yeah, that's

44:07

what it looks like. Okay, great. You

44:08

call it this. We say it uh uh this other

44:11

way, but it but it sort of quickly uh

44:13

settles down to something. Um um so uh

44:18

it's just been it's just been wonderful.

44:20

Um I I think the main thing um uh is to

44:24

just bring them mathematicians and

44:26

physicists uh who actually have common

44:29

interests uh into contact uh really

44:32

really more than anything it's into

44:34

physical contact and uh and talking at a

44:37

blackboard. Um uh uh one of the I think

44:41

this is one of the the kind of stupidest

44:43

things about uh the way um a lot of

44:46

academia is set up uh is uh is to make

44:50

informal interactions that last longer

44:53

than you know 5 hours or two days or a

44:56

week um difficult right uh and some of

45:00

these things just can't you know if

45:02

you've learned a subject in grad school

45:04

and you're talking to someone working in

45:05

an adjacent subject very adjacent

45:08

subject, you can maybe have a

45:10

conversation over lunch and then

45:11

something good can can happen. Um but uh

45:15

if if the if the fields are farther

45:16

apart than that, even a lunchtime

45:18

conversation is probably not enough for

45:20

more than superficial exchange of words

45:22

and ideas and so on. Um I found the sort

45:25

of biggest barrier to uh uh uh working

45:29

in this kind of field is um the kind of

45:32

two weeks, one week, two weeks,

45:34

sometimes a month it takes to learn

45:36

something. Um, and if you have to learn

45:39

it by reading someone's papers, forget

45:40

it. It's not going to take a month. It's

45:42

going to take six months, a year, God

45:43

knows, right? But, um, but you have to

45:45

get together in the same physical

45:47

location at a blackboard and talk for

45:50

uh, a day, two days, a week, however

45:52

long it takes until uh, there's actual

45:55

connection. Um, so it's it's a very

45:58

simple uh, piece of advice about how

46:00

this interaction can be improved, but I

46:02

think it's probably the most practical

46:03

one.

46:04

>> Yeah. So perhaps to wrap it up, um, if

46:06

something comes to mind, do you have a

46:08

favorite anecdote from your days in

46:11

doing research or your own studies that

46:13

comes to mind that you

46:14

>> Oh, there there are way way too many. I

46:17

mean, um, maybe maybe I'll say I'll say

46:20

some I mean, it's it's one it's one

46:22

example. It's one example of uh of many,

46:24

but I I'll I'll I'll maybe say this this

46:27

story because it's illustrative of uh a

46:30

number of the things that we're talking

46:31

about.

46:33

So um uh early on in uh uh in in this

46:37

story with uh uh with with Freddy Kazo

46:40

and my and my students where we're uh

46:43

understanding uh the connection uh

46:46

between uh

46:48

scattering amplitudes for gluons uh the

46:51

work of Andrew Hajes uh and uh some the

46:55

first stumbling into some connection

46:57

with the Gresmanian that kind of blew

46:59

our minds. Um actually the the mini uh

47:02

story there is that uh we didn't know

47:04

what a gross I didn't know what what a

47:05

grossman was but we had um we had uh

47:09

matrices we had these you know we had

47:11

these k byn matrices all over the place

47:13

that were sort of uh we were writing

47:15

them by putting an identity block in one

47:17

side and then some other uh things on

47:19

the other side and then uh you know we

47:21

could do linear transformations um on

47:23

these things we quickly realized

47:25

obviously there was some describing some

47:27

kind of k dimensional plane and and

47:28

dimensions so we knew all of those

47:30

things. I just didn't know the word

47:31

grossman, you know. And at some point as

47:33

we're discussing, uh, you know, Freddy

47:36

and I would would say to each other,

47:37

surely mathematicians know about like,

47:40

you know, planes and n dimensions. Yeah,

47:41

surely. Anyway, uh, Freddy was thumbming

47:45

through Griffith and Harris's algebraic

47:47

geometry book and he just found on some

47:49

page a picture of a k byn matrix with an

47:52

identity block and a bunch of like stars

47:54

and the other entries and he said, "Look

47:56

at this page." you know, he like he

47:58

emailed me, "Look at this page." I'm

48:00

like, "Holy we're like doing a

48:01

we're doing Griffith Harris," you know.

48:04

Uh anyway, um uh but the more the more

48:07

interesting story, so after all all of

48:09

this and we were talking to Pierre

48:10

Delene, who gave us hundred clues and

48:13

Sasha Grov pointed us in the right

48:15

direction. But then we finally ran into

48:17

the work of Alex Basikov who had been

48:19

doing we did not know anything about it.

48:20

We finally ran into the world work of

48:21

Alex Bosikov and I looked at his papers.

48:24

I couldn't make head or tail of them.

48:26

But you see um we had spent uh you know

48:29

6 months at this point starting with a

48:31

picture where we're gluing together

48:33

basic processes where three gluons meet

48:36

and for good reasons you know the the

48:38

the the the gluons two of them can be uh

48:42

uh negative circularly polarized one of

48:44

them positive circularly polarized or

48:45

the other way around. And so we're

48:47

representing the case where two are

48:48

negative one positive with a little

48:50

black vertex and the other one with a

48:51

little white vertex. And so we're

48:53

spending all day long gluing these black

48:55

and white vertices together to make

48:56

pictures that miraculously we found were

48:59

related to these k byn matrices and

49:01

gresmanians and all this stuff. So then

49:04

we found out that this posikov guy uh

49:06

also had these matrices and was saying

49:08

lots of interesting things about them

49:10

clearly seemed related somehow. So we

49:12

the whole crew of us uh drove up uh to

49:15

talk to him at uh uh MIT. So got to MIT

49:19

we met him for the first time. Wonderful

49:20

guy, amazing guy. still uh still great

49:23

great great great friends with them. Um

49:26

but it was very exciting. We spent the

49:27

whole morning, you know, we had our

49:28

matrices like, yeah, they look like my

49:30

my matrices and okay, we're clearly

49:32

saying the same thing. Mind-blowing.

49:33

Fantastic. But uh only about these

49:36

matrices and all these sort of algebraic

49:38

structures only about these matrices.

49:39

And then um then we went to lunch and

49:43

and uh uh in all the excitement, Alex is

49:46

like, you know, I'm a little surprised

49:47

though in my way of thinking about

49:49

things. there's some very important

49:51

pictures that go along with these uh

49:53

with these uh with these matrices. And

49:56

we're like, "Oh yeah, you know, what do

49:57

they look like?" He said, "They look

49:58

like this." And we drew like we drew one

50:00

of the pictures that's like literally on

50:01

our board like over and over and over

50:03

again for the past 3 months. Uh of

50:06

course interpreted in totally different

50:07

ways which we had been deliberately

50:09

hiding from him because you know we

50:11

thought that was that was the physics

50:13

part you know so we don't want to we

50:14

don't want to bore you with these

50:15

pictures but let's get to these matrices

50:17

and the aggressmanion. But that was

50:19

where it came from for him as well. And

50:21

then he pointed us back to his paper um

50:23

where he has this throwaway comment that

50:25

perhaps we can think about the little

50:27

black and white vertices as something to

50:28

do with finding diagrams. It's

50:31

completely insane thing that of course

50:33

ended up to be not quite fine diagram.

50:35

It ended up being totally true, right?

50:37

Um that sort of thing has happened a

50:39

number of times. It's a it's a it's a

50:41

great story because it it illustrates so

50:43

much this point that you run into the

50:45

same beast. But I'll never forget that

50:47

that uh one of the great things about

50:49

Alex um you know um the one the one uh

50:52

the one distinction I'll make amongst

50:55

mathematicians there are some

50:56

mathematicians when you ask for an

50:57

example they give you the tiniest most

51:00

trivial example right and then for me as

51:02

a physicist it's hard to understand

51:04

something from the dead simplest example

51:06

um you need to see maybe the second or

51:08

third most complicated examples before

51:10

you see something going on and uh Alex

51:12

bless his heart always starts with the

51:14

second or third most complicated example

51:16

to illustrate something. And so he

51:18

happened to draw a picture that was a

51:19

sort of pentagon box. Um, and it was

51:22

just shocked us that it was exactly the

51:24

pictures that we've been drawing for

51:26

such such a long time.

Interactive Summary

This video features a discussion with Nema Kani Hamemed, a theoretical physicist, about his journey into physics, his inspirations, and his research. He shares how his childhood fascination with nature and a rebellion against his physicist parents led him to the field. A pivotal moment was understanding the concept of escape velocity at age 12, which revealed the power of mathematics in explaining the natural world. Nema emphasizes the importance of role models who are accessible and relatable, rather than distant "gods" of physics. He highlights his high school physics teacher, John Wy, who introduced him to the Lagrangian and partial derivatives, fundamentally changing his understanding of physics. His research interests evolved from particle physics and the mystery of the universe's size to exploring the concept of naturalness and the multiverse. A significant part of the discussion revolves around his work on scattering amplitudes, particularly the development of the "amplitron." He explains the deep connections emerging between theoretical physics, cosmology, and mathematics, particularly in areas like Grassmannians and combinatorics. Nema expresses excitement about the ongoing interdisciplinary research, emphasizing the need for physicists and mathematicians to collaborate closely, often at a blackboard. He concludes by sharing an anecdote about discovering the connection between his work on gluon scattering amplitudes and the mathematical concept of Grassmannians, illustrating the surprising ways different fields can intersect.

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