The Relativistic Quantum World
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The Relativistic Quantum World. A lecture series on relativity theory and quantum mechanics. Marcel Merk. University of Maastricht, Sept 16 – Oct 7, 2013. The Relativistic Quantum World. Sept 16: Lecture 1: The Principle of Relativity and the Speed of Light

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A lecture series on relativity theory and quantum mechanics

The Relativistic Quantum World

A lecture series on relativity theory and quantum mechanics

Marcel Merk

University of Maastricht, Sept 16 – Oct 7, 2013


The relativistic quantum world

The Relativistic Quantum World

Sept 16:

Lecture 1: The Principle of Relativity and the Speed of Light

Lecture 2: Time Dilation and Lorentz Contraction

Sep 23:

Lecture 3: The Lorentz Transformation

Relativity

Lecture 4: The Early Quantum Theory

Sep 30:

Lecture 5: The Double Slit Experiment

Lecture 6: Quantum Reality

Quantum

Mechanics

Oct 7:

Lecture 7: The Standard Model

Lecture 8: The Large Hadron Collider

Standard

Model

Lecture notes, written for this course, are available: www.nikhef.nl/~i93/Teaching/

Literature used: see lecture notes.

Prerequisite for the course: High school level mathematics.


The story sofar

The Story Sofar

Postulates of Special Relativity

Two observers in so-called Inertial frames, i.e. they move with a constant relative speed to each other:

The laws of physics for each observer are the same

The speed of light in vacuum for each observer is the same

“Absolute velocity” is meaningless


The story sofar1

The Story Sofar

Time dilation:

Lorentz contraction:

g

Speed v/c


Real life example

Real life example

  • Muon particles have a half-lifetime of 1.56 μs.

  • In the atmosphere they are created at 10 km height with a speed: v = 0.98 c

  • They can reach the surface because:

  • As seen from an observer on earth

  • they live a factor 5 longer

  • As seen from the muon particle the

  • distance is a factor 5 shorter


A lecture series on relativity theory and quantum mechanics

Lecture 3

The Lorentz Transformation

  • “Imagination is more important than knowledge.”

  • Albert Einstein


Coordinate systems

Coordinate Systems

“Do not worry about your difficulties in mathematics. I can assure you mine are still greater.”

-Albert Einstein

A reference system or coordinate system is used to determine the time and position of an event.

Reference system S is linked to observer Alice at position (x,y,z) = (0,0,0)

An event is fully specified by giving its coordinates and time: (t, x, y, z)

Reference system S’ is linked to observer Bob who is moving with velocity v with respect to Alice. The event has: (t’, x’, y’, z’)

How are the coordinates of an event, say a lightning stroke in a tree, expressed in coordinates for Alice and for Bob?

(t, x, y, z) (t’, x’, y’, z’)


Space time diagram

Space-time diagram

Bob drives from Maastricht to Amsterdam with 100 km/h

Alice drives from Maastricht to Amsterdam with 200 km/h

t

“Events”:

12h00

Departure Alice & Bob

1 h

Arrival Bob

Arrival Alice

11h00

“World lines”:

1 h

Bob’s world-line

Alice’s world-line

(x,t)

10h00

x

200 km

Amsterdam

Maastricht

Events with space-time coordinates: (x,t)

More general: it is a 4-dimensional space: (x,y,z,t)


Coordinate transformation

Coordinate transformation

How does Alice’s trip look like in the coordinates of the reference system of Bob?

t

t’

12h00

12h00

1 h

1 h

(x2,t2)

(x2’,t2’)

11h00

11h00

1 h

1 h

(x1’,t1’)

(x1,t1)

10h00

x

10h00

x’

200 km

100 km

Alice as seen from Maastricht

S = fixed reference system in Maastricht

Alice as seen from Bob

S’ = fixed reference to Bob


Coordinate transformation1

Coordinate transformation

How does Alice’s trip look like in the coordinates of the reference system of Bob?

t

t’

12h00

12h00

1 h

1 h

(x2,t2)

(x2’,t2’)

11h00

11h00

1 h

1 h

(x1’,t1’)

(x1,t1)

10h00

x

10h00

x’

Classical (Galilei transformation):

Relativistic (Lorentz Transformation):

200 km

100 km

with:


Lorentz transformations

Lorentz Transformations

Hendrik Anton Lorentz (1853 – 1928)

Dutch Physicist in Leiden

(Nobelprize 1902 with Pieter Zeeman)

To explain the Michelson-Morley experiment he assumed that bodies contracted due to intermolecular forces as they were moving through aether.

(He believed in the existence if the aether)

Einstein derived it from the relativity principle and also saw that time has to be modified.


Let s go crazy and derive it

Let’s go crazy and derive it…


Classical limit

Classical Limit

Lorentz Transformation:

With the new variables:

fraction of light-speed

Relativistic factor

It becomes:

For every day life experience:

velocities much less than lightspeed

In every day life we do not see the

difference between the classical and

the relativity theory


Relativity revisited

Relativity Revisited


Paradoxes case 1 sherlock watson

Paradoxes Case 1 : Sherlock & Watson

A murder scene being investigated.

Alice enters a room and from the doorstep shoots Bob, who dies. (Thought experiment!)

Sherlock stands at the doorstep (next to Alice) and observes the events.

Alice shoots at t = tA from position x = xA

Bob dies at t = tBat position x = xB

Watsonpasses by on a fast train and sees the same scene. He sees:

Alice shoots at t’ = tA’ from position x’ = xA’

Bob dies at t’ = tB’ at position x’ = xB’


Causality

Causality

Sherlock: Alice shoots at Bob from xA at time tA

Bob dies on position xB and time tB

What does Watson see at v=0.6c?

ct

ct’

(xB,ctB)

ctB

(xA’,ctA’)

(xB’,ctB’)

(xA,ctA)

0

x

x’

To make the calculation easy let’s take xA = 0 and tA = 0 :

xB

0

This is what Watson sees:

0

ctB’

If distance xB > ctB / 0.6 then ctB‘ < 0 :

Bob dies before Alice shoots the gun!

xB’

0


What is wrong

What is wrong?

The situation was not possible to begin with!

Light-speed

ct

Time-like

Space-like

(xB,ctB)

(xA,ctA)

0

x

0

Nothing can travel faster then the speed of light, also not the bullet of gun.

The requirement: xB > ctB / 0.6 implies a speed v = xB/tB > c / 0.6 = 1.67 c !

Causality is not affected by the relativity theory!


Paradox 2 a ladder in a barn

Paradox 2: A ladder in a barn?

Alice runs towards a barn with

v = 0.8 c (g =1.66).

She carries a 5 m long ladder.

Bob stands next to 4 m deep barn.

Will the ladder fit inside?

4 meters

5 meters

Alice: no way!

She sees a L/g = 2.4 m deep shed

Bob: sure, no problem!

He sees a L/g = 3 m long ladder


Paradox 2 a ladder in a barn1

Paradox 2: A ladder in a barn?

Alice’s experiment:

Bob’s experiment:

Bob and Alice don’t agree on simultaneity of events.

Alice claims the back door is opened before the front door is closed.

Bob claims both doors are closed at the same time.

*But will it stay inside?!

To stay inside the ladder must stop (negative accelleration)

Compressibility lightspeed

The ladder has been

fully inside

The ladder has not been fully inside


Paradox 3 the twin paradox

Paradox 3: The Twin Paradox

Identical twins:

Jim andJules

Jules

Jim

“Jules+2y”

“Jim+10y”

Jules travels to a star with v = 99.5% of c (g = 10) and returns to Jim on earth after a trip of one year. Jim has aged 10 years, Jules only 1 year.

Jim understands this. Due to Jules’ high speed time went slower by a factor of 10 and therefore Jim has aged more than Jules.

But Jules argues: the only thing that matters is our relative speed!

As seen from his spaceship time goes slower on earth! He claims Jim should be younger!

Who is right?

Answer: special relativity holds for constant relative velocities.

When Jules turns around he slows down, turns and accelerates back.

At that point time on earth progresses fast for him, so that Jim is right in the end.


Paradox 3 the twin paradox1

Paradox 3: The Twin Paradox

  • 1971: A real experiment!

  • Joseph Hafele & Richard Keating tested it with 3 atomic cesium clocks.

  • One clock in a plane westward around the earth (against earth rotation)

  • One clock in a plane eastward around the earth (with earth rotation)

  • One clock stayed behind in the lab.

The clock that went eastward was 300 nsec behind, in agreement with relativity.


Addition of velocities

Addition of Velocities .

w=

v=

With which speed do the ball and the outfielder approach each other?

Intuitive law (daily experience): 30 m/s+10 m/s=40 m/s

Galileo Galilei

More formal:

Observer S (the Batter) observes the ball with relative velocity: w

Observer S’ (the running Outfielder) observes the ball with relative velocity: w’

If the velocity of S’ with respect to S is: v

This is the Galileian law for adding velocities.

What is the relativistic correct formula?

w’=w+v


Derive the laws for adding speed

Derive the laws for adding speed .

Lorentz Transformation:

Galilei Transformation:


Relativistic transformation law

Relativistic Transformation law . .

w=

v=

Relativistic:

0.8c

0.6c

Bob in a rocket passes a star with 0.8 c

Alice in a rocket passes a star with 0.6 c

In opposite directions.

What is their relative speed?


How about alice seeing light from bob

How about Alice seeing light from Bob?

How fast does the light go for Alice?


E mc 2

E=mc2

Consider a box with length L and mass M floating in deep space.

A photon is emitted from the left wall and a bit later absorbed in the right wall.

Center of Mass (CoM) of box + photon must stay unchanged.

Action = - Reaction: photon momentum is balanced with box momentum

Time it takes the foton

Distance that the box has moved

C.O.M. does not move: box compensated by photon C.O.M.

Substitute the above equations

Equivalence of mass and energy!


Conclusions relativity

Conclusions Relativity

  • Simple principle:

  • Laws of physics of inertial frames are the same.

  • Speed of light is the same for all observers.

  • Consequences:

  • Space and time are seen differently for different observers.

  • Bob’s time is a mixture of Alice’s time and space and vice versa.

  • Bob’s space is a mixture of Alice’s time and space and vice versa.

  • Time dilation and Lorentz contraction

  • Energy and mass are equivalent

General Relativity: inertial mass = gravitational mass


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