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High-Temperature Superconductivity Understood at Last

High-Temperature Superconductivity Understood at Last

Released Wednesday, 1st February 2023
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High-Temperature Superconductivity Understood at Last

High-Temperature Superconductivity Understood at Last

High-Temperature Superconductivity Understood at Last

High-Temperature Superconductivity Understood at Last

Wednesday, 1st February 2023
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0:04

Welcome to Quanta Magazine's podcast.

0:07

Each episode, we bring you stories about

0:09

developments and science and mathematics. I'm

0:12

Susan ballot. For decades,

0:14

a family of crystals has stumped

0:16

physicists with its baffling

0:18

ability to superconduct electricity

0:21

at far warmer temperatures than

0:23

other materials. But now,

0:26

an atomic scale experiment sheds

0:28

new light on this mystery. That's

0:31

next. Quanta

0:36

is an editorially independent online

0:39

publication supported by the Simon's

0:41

Foundation. To enhance public

0:43

understanding of science. We

0:49

now finally know why a family of

0:52

crystals can perfectly conduct

0:54

an electric current at far

0:56

warmer temperatures than other materials.

0:59

That's because an experiment years in

1:01

the making has directly visualized

1:04

super conductivity on the atomic

1:06

scale in one of those crystals. Electrons

1:09

appear to nudge each other into a

1:11

frictionless flow in a matter first

1:13

suggested by a theory nearly as

1:15

old as the mystery itself. Siberiasachdev,

1:18

a physicist at Harvard University who

1:21

builds theories of the crystals known

1:23

as Coup rates, says the evidence

1:25

is beautiful and direct. Such

1:28

dev wasn't involved in the experiment. JC

1:31

Seamus Davis led the new experiment

1:34

at the University of

1:35

Oxford. He talked with reporter, Charlie

1:37

Wood. It

1:38

was it was really exciting, actually.

1:41

Since I've worked on this problem for twenty five

1:43

years, and I hope I have solved it. I have

1:45

absolutely really

1:46

not. I would like to do something else. The

1:48

new measurement matches prediction based

1:51

on the theory, which attributes Superconductivity

1:55

to a quantum phenomenon called

1:57

super exchange. Andre

1:59

Marie Trimblay is a physicist at

2:02

the University of Sherbrooke in Canada

2:04

and the leader of the group that made the prediction

2:06

in twenty twenty

2:07

one.

2:08

I'm amazed by the quantitative agreement.

2:11

I'm surprised that this this that

2:13

is working so well. The research advances

2:16

the perennial ambition of the field.

2:18

To take cuprate super conductivity,

2:21

and strengthen its underlying mechanism

2:24

in order to design world changing materials

2:27

capable of electricity

2:29

at even higher temperatures. Room

2:31

temperature superconductivity would

2:34

bring perfect efficiency to everyday

2:36

electronics, power lines, and

2:38

more. But real world uses

2:41

are still pretty far

2:42

off. Davis talked with Charlie

2:44

Wood about the super exchange theory.

2:46

If this class of theory is correct,

2:49

and it should be possible to describe

2:51

synthetic materials with different

2:53

atoms at different locations in

2:55

which charge transfer super exchanges the

2:58

mechanism. For which the temperature

3:00

is higher.

3:01

Physicists have struggled with super

3:03

conductivity since it was first observed

3:06

in nineteen eleven. Dutch

3:08

scientist, Heike Comerling Ones,

3:11

and collaborators cooled a

3:13

mercury wire to about four

3:15

kelvins that's four degrees

3:17

above absolute zero. They

3:19

watched with astonishment as the

3:21

electrical resistance plummeted

3:24

to zero. Electrons definitely

3:27

winded their way through the wire

3:29

without generating heat when they

3:31

collided with its atoms, the origin

3:33

of resistance. Davis says

3:35

it would take a lifetime of effort to figure

3:37

out how. John Gardein,

3:40

Leon Cooper, and John Robert

3:42

Shrieffer, cracked the case by

3:44

building on key experimental insights

3:47

from the mid nineteen fifties. They

3:49

published their Nobel prize winning

3:51

theory of this conventional form

3:53

of super conductivity in nineteen

3:55

fifty seven. BCS theory,

3:58

as it's known today, holds that

4:00

vibrations moving through rows of atoms

4:03

glue electrons together as

4:06

a negatively charged electron flies

4:08

between atoms it draws the positively

4:11

charged atomic nuclei toward

4:13

it and sets off a ripple. That

4:16

ripple pulls in a second electron

4:19

Overcoming their fierce electrical repulsion,

4:22

the two electrons form what's called

4:24

a Cooper pair. Jorg Schmallian

4:27

is a physicist at the Karlsrure Institute

4:30

of Technology in

4:31

Germany. It is true trickery

4:33

of nature because this group of peers

4:35

not supposed to happen because these are

4:37

all reports of energies. But

4:40

what the system does is the wave function

4:42

of this pair as a whole has

4:44

a triglycerid or change its sign

4:46

in just such a way that it makes

4:48

in a repulsion to

4:50

attract. When electrons coupled up,

4:52

Further quantum trickery makes super

4:54

conductivity unavoidable. Normally,

4:57

electrons can't overlap, but

4:59

Cooper pairs follow a different quantum

5:02

mechanical rule. They act

5:04

like particles of light, any

5:06

number of which can pile the head

5:08

of a pin. Many Cooper

5:10

Pears come together and merge into

5:12

a single quantum mechanical state

5:14

known as a superfluid. Which becomes

5:16

oblivious to the atoms it passes

5:18

between. BCS theory

5:20

also explained why mercury and

5:23

most other metallic elements superconduct

5:26

when cooled close to absolute zero,

5:28

but stop doing so above a few

5:30

kelvins. Atomic ripples

5:33

make for the febalest of glues. Turn

5:35

up the heat and jiggles atoms and

5:38

washes out the lattice vibrations. Then

5:41

in nineteen eighty six, IBM

5:43

researchers Gayorg Bed Nords

5:45

and Alex Mueller stumbled onto

5:47

a stronger electron glue in

5:50

coup rates crystals consisting

5:52

of sheets of copper and oxygen interspersed

5:55

between layers of other elements. After

5:58

they observed a cuprate superconducting at

6:00

thirty kelvins, where researchers soon

6:03

found others that above

6:05

one hundred and then above one hundred

6:07

thirty kelvins. The breakthrough

6:09

launched a widespread effort to

6:11

understand the tougher glue responsible

6:14

for this high temperature super conductivity.

6:18

Perhaps electrons bunched together

6:20

to create patchy whippling concentrations

6:23

of charge or maybe they interacted

6:25

through spin an intrinsic property

6:28

of the electron that oriented in

6:30

a particular direction, like a quantum

6:32

sized magnet. The late

6:34

Philip Anderson, an American Nobel

6:37

laureate, an all around legend in

6:39

condensed matter physics, put

6:41

forth the theory just months after

6:43

high temperature superconductivity was

6:46

discovered. He argued that at

6:48

the heart of the glue, Leia previously

6:50

described quantum phenomenon called

6:53

super exchange, a force

6:55

arising from electrons ability

6:57

to hop. When electrons

7:00

can hop between multiple locations,

7:02

their position at any one moment

7:05

becomes uncertain, while their

7:07

momentum becomes precisely defined.

7:10

A sharper momentum can be a

7:12

lower momentum and therefore a

7:14

lower energy state which particles

7:16

naturally seek out. The

7:19

upshot is that electrons seek

7:21

situations in which they can hop.

7:23

For instance, an electron prefers

7:25

to point down when its neighbor points

7:28

up, since this distinction allows

7:30

the two electrons to hop between

7:32

the same atoms. In this way,

7:34

super exchange establishes a

7:37

regular up down up

7:39

down pattern of electron spins

7:41

in some materials. It also

7:43

nudges electrons to stay a certain

7:45

distance apart. If they're too

7:47

far apart, they can't hop.

7:50

It's this effective attraction that Anderson

7:52

believed could form strong Hooper

7:55

pairs. Experimentalists long

7:58

struggled to test theories like Andersons.

8:01

Material properties that they could measure,

8:03

like reflectivity or resistance offered

8:06

only crude Summaries of the collective

8:08

behavior of trillions of electrons,

8:11

not pairs. Here's Davis again.

8:13

It's a deep, deep problem of physics.

8:16

So we don't really have sharp

8:18

guidance on what we're supposed to do. And

8:21

none of the traditional

8:22

techniques of condensed matter physics were

8:25

ever designed to solve a problem like this.

8:27

Davis is an Irish physicist with

8:29

labs at Oxford Cornell University,

8:32

University College Cork, in

8:34

the International Max Planck Research

8:37

School for Chemistry and Physics of

8:39

Quantum Materials in Dresden, Germany.

8:42

He's gradually developed tools to

8:44

scrutinize coup rates on the

8:46

atomic level. Earlier experiments

8:48

gauged the strength of a material superconductivity

8:52

by chilling it until it reached the

8:54

critical temperature where superconductivity began.

8:58

With warmer temperatures indicating stronger

9:00

glue. But over the last decade,

9:03

Davis' group has refined a way

9:05

to prog the glue around individual

9:08

atoms. They modified an

9:10

established technique called scanning

9:13

tunneling microscopy which

9:15

drags a needle across a surface

9:17

measuring the current of electrons leaping

9:20

between the two. By swapping

9:22

the needle's normal metallic tip

9:24

for a superconducting tip and

9:26

sweeping it across a coup rate,

9:28

they measured a current of electron pairs

9:31

rather than individuals. This

9:33

let them map the density of

9:35

Cooper pairs surrounding each atom,

9:37

a direct measure of They

9:41

published the first image of swarms

9:43

of Cooper Pairs in nature in two thousand

9:45

sixteen. That same

9:47

year, an experiment by Chinese physicist

9:50

provided a major piece of evidence

9:52

supporting Anderson's super exchange

9:55

theory. They showed that

9:57

the easier it is for electrons to

9:59

between copper and oxygen atoms

10:02

in a given cuprate, the higher

10:04

the cuprate's critical temperature. And

10:06

that means the stronger it's glue. Davis

10:09

and his colleague sought to combine the two

10:11

approaches in a single cuprate crystal

10:14

to more conclusively reveal the

10:16

nature of the

10:17

glue. Here's Davis again. So

10:19

about two years ago in a kind of

10:21

aha moment, Actually, in the

10:23

Zoom group

10:23

meeting, we realized this

10:26

experiment is possible. It dawned on

10:28

the researchers that a cup rate called

10:30

bismuth Strontium, calcium, copper

10:33

oxide, or Bisco for

10:35

short, had a peculiar feature

10:37

that made their dream experiment possible.

10:40

In Bisco, surrounding sheets

10:42

of atoms squeeze the layers of

10:44

copper and oxygen atoms into a

10:46

wavy pattern. This varies

10:48

the distance between certain atoms,

10:50

which in turn affects the energy required

10:53

to hop. The variation causes

10:55

headaches for theories. Who like

10:58

their lattice's tidy, but

11:00

it gave the experimentalists exactly

11:02

what they needed, a range of

11:04

hopping energies in one sample.

11:07

They used a traditional scanning microscope

11:10

with a metal tip to stick electrons

11:12

onto some atoms and pluck them from

11:14

others. Mapping the hopping energies

11:17

across the Kooprate. They then

11:19

swapped in a Kooprate tip to measure

11:21

the density of Koopa pairs around

11:23

each atom. The two maps

11:25

lined up. Where electrons struggled

11:28

to hop, super conductivity was

11:30

weak. Where hopping was Superconductivity

11:34

was strong. The relationship between

11:36

hopping energy and Cooper paired

11:38

density closely matched a sophisticated

11:41

numerical prediction from twenty twenty

11:44

one by Trimblay and his colleagues,

11:46

which argued that this relationship should

11:49

follow from Anderson's theory. Davis

11:51

is finding that hopping energy is linked

11:54

with super conductivity strength was

11:56

published in twenty twenty two the

11:58

proceedings of the National Academy of

12:00

Sciences. It strongly implies

12:03

that super exchange is the superglue

12:06

enabling high temperature Superconductivity. Ali

12:10

Yazdani is a physicist at Princeton

12:12

Universe who's developed similar

12:14

techniques to study coup rates and other

12:17

exotic instances of super conductivity

12:20

in parallel with Davis' group. This

12:22

idea has been around a long time. It's

12:24

a nice piece of work because it brings new

12:26

technique to further show that this

12:28

idea has legs. That's as far as would

12:30

go. You know, in size, you have to be careful

12:33

between causation and

12:34

correlation. And then, you know,

12:37

turning the thing on his head and predicting

12:39

the next thing. Yazdani and other researchers

12:41

cautioned that there's still a chance, however,

12:44

remote, that glue strength

12:46

and ease of hopping move and

12:48

lock step for some other reason

12:50

and that the field is falling into the classic

12:53

correlation equals causation trap.

12:56

For Yazdani, the real way to prove

12:58

a causal relationship will be to

13:00

harness super exchange to

13:02

engineer some flashy new superconductors.

13:06

Super Exchange isn't a new idea.

13:08

So plenty of researchers have already thought

13:10

about how to fortify it. Perhaps

13:13

by further squishing the copper and

13:15

oxygen lattice or experimenting

13:17

with other pairs of elements. You

13:19

remember Andre Marie Trimblay, a

13:22

physicist at the University of Sherbrooke

13:24

in

13:24

Canada.

13:25

There are already predictions on the

13:27

table. Of course, sketching atomic

13:29

blueprints and designing materials

13:31

that do what researchers want isn't

13:34

quick or easy. Plus,

13:36

there's no guarantee that even bespoke

13:38

Coop rates will achieve critical temperatures

13:41

much higher than those of the Coop rates

13:43

we already know. The strength

13:45

of super exchange could have a

13:47

hard ceiling just as atomic vibrations

13:50

seem to. Some researchers are

13:52

investigating candidates for tirely

13:54

different and potentially even stronger

13:56

types of glue. Others leverage

13:59

unearthly pressures to shore up

14:01

the traditional atomic vibrations. But

14:04

Davis' result could energize and

14:06

focus the efforts of chemists and material

14:08

scientists who aim to lift

14:11

coup rate superconductors

14:12

to greater heights. York

14:14

Schmale says scientists are already

14:17

working on ideas. The creativity of

14:19

people who need design materials is

14:21

limitless. But these are hard

14:24

experiments that cost not just

14:26

money, but also, you know, students

14:28

careers and lifetimes. So therefore,

14:31

the more confident we are that certain

14:33

mechanism is the right one, the more

14:35

natural it is invest further into

14:37

this one.

14:43

Matt Carlstrom helped with this episode. I'm

14:45

Susan ballot. For more on this story,

14:48

read Charlie Woods' full article. High

14:50

temperature super conductivity understood

14:53

at last. On our website, quantum

14:55

magazine dot org. Explore

14:58

math mysteries in the Quanta book, The

15:00

Prime Number Insperacy, published

15:02

by the MIT Press. Available

15:04

now at amazon dot com, barnes and noble

15:06

dot com, or your local bookstore. Also,

15:09

make sure to tell your friends about the Quanta magazine

15:12

Science podcast then give us a positive

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