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B1 중급 영어 20:00 Educational

Parallel Worlds Probably Exist. Here’s Why

Veritasium · 24,620,101 조회수 · 추가됨 2일 전

학습 통계

B1

CEFR 레벨

5/10

난이도

자막 (535 세그먼트)

00:00

a portion of this video was sponsored by

00:01

Norton 360 classical mechanics is great

00:05

if you know the state of a system say

00:08

the position and velocity of a particle

00:10

then you can use an equation Newton's

00:12

second law to calculate what that

00:14

particle will do in the future in

00:16

quantum mechanics if you know the

00:18

quantum state of a particle that is its

00:21

wave function you can use the

00:22

Schrodinger equation to calculate what

00:24

that particle will do in the future

00:26

usually it spreads out over time as it

00:29

is doing here note to make this

00:31

animation we really solved the

00:34

Schrodinger equation so there's a

00:36

beautiful symmetry here if you know the

00:38

initial state you can use an equation to

00:41

evolve that state smoothly and

00:43

continuously into the future the problem

00:46

is in quantum mechanics we never

00:48

actually observe the wave function like

00:50

this instead when we measure it we find

00:53

the particle at a single point in space

00:56

so how are we to reconcile the

00:58

spread-out wavefunction evolving

01:00

smoothly under the Schrodinger equation

01:02

with this point like particle detection

01:04

now I think it's understandable that

01:07

when the founders of quantum theory

01:09

approached this problem they considered

01:11

the measurement more real than the

01:13

wavefunction after all the measurement

01:16

was something we had actually observed

01:18

and it matches our experience of a world

01:21

of matter particles it was harder to say

01:24

what the wavefunction was exactly

01:26

Schrodinger formulated his wave equation

01:29

because scientists notably debroglie

01:31

suspected that matter has wave-like

01:33

properties but it took a third physicist

01:36

Max Born to propose how we should

01:39

interpret the wave function at each

01:41

point in space the wave function has a

01:43

complex amplitude essentially just a

01:46

real number plus an imaginary number Max

01:48

Born suggested if you take that

01:50

amplitude and square it you get the

01:52

probability of finding the particle

01:54

there the fact that you have to square

01:57

the amplitude actually appears as a last

01:59

minute footnote in boran's paper but

02:01

that is how probability was introduced

02:04

into the core of our picture of reality

02:07

that's a pretty big philosophical leap I

02:09

mean no longer is the universe

02:11

deterministic

02:12

this made a lot of scientists especially

02:14

Einstein uncomfortable but the born rule

02:17

as it is now called remains at the heart

02:19

of quantum mechanics because it is

02:21

spectacularly successful at predicting

02:23

the outcomes of experiments so the way

02:26

quantum mechanics came to be understood

02:27

and the way I learned it is that there

02:29

are two sets of rules when you're not

02:32

looking the wave function simply evolves

02:34

according to the Schrodinger equation

02:35

but when you are looking when you make a

02:38

measurement the wavefunction collapses

02:40

suddenly and irreversibly and the

02:42

probability of measuring any particular

02:44

outcome is given by the amplitude of the

02:47

wave function associated with that

02:48

outcome squared now Schrodinger himself

02:51

hated this formulation which is actually

02:54

why he invented the famous Schrodinger's

02:57

cat thought experiment put a cat in a

02:59

box with a radioactive atom add a

03:02

radiation detector that triggers the

03:04

release of poisonous cyanide gas now

03:07

although it was only meant as a thought

03:09

experiment Schrodinger helpfully notes

03:11

this device must be secured against

03:14

direct interference by the cat anyway

03:16

the whole point of the experiment is to

03:19

magnify the state of the atom up to the

03:20

state of something macroscopic and

03:22

tangible he could have picked anything

03:24

it didn't have to be alive but

03:26

Schrodinger selected a cat if the atom

03:29

decays the detector detects radiation

03:32

releases the poison and the cat dies if

03:35

the atom doesn't decay the detector

03:37

doesn't detect radiation poison is not

03:39

released and the cat remains alive since

03:42

the state of the cat and detector

03:43

apparatus are directly tied to the state

03:46

of the atom we say they are entangled

03:49

where things get weird is that according

03:51

to quantum mechanics the state of the

03:53

atom does not have to be either decayed

03:55

or not decayed generally it's in a

03:57

superposition of both decayed and not

04:00

decayed at the same time assuming no

04:02

measurements have been made this

04:04

superposition state of the atom gets

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