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Title: ON THE ROAD AGAIN


1
ON THE ROAD AGAIN
  • Final Destination Quantum Mechanics

2
Taking the Trip From Classical Physics to Quantum
Mechanics
  • What is Quantum Mechanics one may ask? Well, in a
    nutshell, quantum mechanics is
  • The FUNdamental branch of physics replacing
    classical Newtonian Mechanics and
    Electromagnetism at the atomic and subatomic
    levels.
  • Quantum mechanics provides explanations for many
    phenomena that are unattainable through classical
    mechanics
  • Namely quantization, wave particle duality,
    the uncertainty principle, quantum entanglement

3
Dont be fooled, this will be no short trip
  • Quantum theory ideas did not originate overnight.
    There were numerous experiments and observed
    phenomena that eventually led to this modern way
    of thought.
  • The move from General Relativity to Quantum
    mechanics is a huge step, since the two theories
    seemingly contradict each other. The two
    fundamental issues yielding this contradiction
    are
  • Classical is essentially a deterministic approach
    while quantum mechanics is essentially
    indeterministic
  • General relativity relies mainly on gravity while
    quantum mechanics relies on three fundamental
    forces, the strong, weak, and electromagnetic.
  • (though these forces are imperative in Quantum
    Theory, we will leave out a discussion of them
    here, for they will be covered in a latter
    presentation) For the remainder.. We will look
    at the major players on the road to the discovery
    and development of this way of thought.)

4
Why are we going here?
  • Two fundamental discrepancies between
    experimental observations and classical physics
    were noticed in the late 1800s.
  • These two discrepancies (namely the ultra
    violet catastrophe and the discrete spectral line
    phenomena) caused scientist to re-examine several
    established ideas and arrive at a new way of
    thought.

5
EVERYONE JUMP IN THE VAN! Were hittin the road!
  • Problem 1 Energy and Blackbody radiation
  • Intro
  • A black body is a surface which absorbs all
    radiation and at a given temperature T, can also
    emit radiation
  • Thus, using the ?(?,T) energy function, holding T
    constant, the individual wavelengths ? of the
    radiation can be analyzed
  • At the turn of the 20th century, this in fact was
    done and the observations were first recorded by
    Otto Lummer and Ernst Pringsheim and then again
    the following year by Heinrich Rubens and
    Ferdinand Kurlbaum
  • The results gathered are shown in the following
    figure

6
Results
7
Uh Oh!
  • According to the Equipartition Theorem (a
    non-quantum theorem) every degree of freedom of a
    system must share equally in the energy available
    to the system,
  • Take for example, a blackbody radiation of
    dimension l , then we know that wavelengths are
    given by ? (2l )/ n, where n 1,2,3 .
  • Each of these represent a degree of freedom, and
    therefore, by the equipartition theorem, should
    share the energy equally.
  • Thus, since there are infinitely many waves as
    the wavelength gets shorter, it would be assumed
    that the majority of the light (ie radiation)
    would be at the short wavelength end of the
    spectrum, as shown by the dotted line

8
  • Notice the dotted line

9
Why is this a problem?Lets do the math
  • A major problem arises, since we know from
    derivations that follow directly from the
    equipartition theorem, done by Rayleigh and Sir
    James Jeans, that through classical analysis, the
    energy density function can be expressed as


  • where k is
    Boltzmanns constant
  • But it is easily seen that by applying basic
    calculus the limit
  • of as ?
    approaches 0, is infinity. Obviously
  • contradicting the observed results shown in
    the figure by the solid line. If this were
    indeed the case, the results would be described
    by the dotted line in the previous figure.
  • This discrepancy and blow up at short
    wavelengths is often referred to as the
    ultra-violet catastrophe and spurred much
    thought as to how to remedy it.

10
FLAT TIRE!!Our classic car is getting old, time
to trade it in
  • The discrepancy between the observational results
    and this equation is an intense problem. Since
    the energy density equation derived by Jeans in
    1905, followed directly from the well established
    equipartition theorem, which was a consequence of
    general relatively. Thus because these do not
    correlate, it implies that the overlying theory
    must be inadequate.

11
Problem 1 Flat Tirenow we have Problem 2
running out of gas
  • The second phenomena leading to quantum theory
    stems from the pattern of spectral lines emitted
    by an element
  • When an electric arc passes through a sample of
    gas, it is observed that only certain frequencies
    of light are present.
  • When observing the spectral lines by separating
    them with a prism, it is observed that the
    wavelengths are distinct to the element emitting
    the spectrum

12
Whats so bad about that?
  • This observation directly contradicts the
    predictions of classical physics
  • According to classical physics, accelerated
    particles must emit electromagnetic radiation,
    and thus if they were moving randomly within the
    atom, all the spectra would be emitted, thus
    producing a continuous spectrum, however the
    results showed a discrete distribution.
  • Due to this phenomena, scientist began
    associating these spectral emission with stable
    orbits, and an empirical formula was even
    discovered through trial and error efforts, to
    fit the observed reality.
  • This equation is
  • v R(1/m2 1/n2) known as Balmers Eq.
  • where v is the velocity of frequencies of
    the lines, R is a universal constant, m is a
    constant representing a particular series, and n
    is an integer representing a particular line

13
What are we going to do?
  • Many models of the atom where constructed to try
    to describe this phenomena. However, they nearly
    all assumed a uniform distribution of the
    positive charge.
  • However, in 1909, Hans Greiger and Ernst Marsden
    disproved this theory through careful examination
    of the scattering of a beam of charged particles.
    What would be expected if the previous models
    were in fact reality, would have been a uniform
    scattering of the particles. However this was
    not the case

14
What happened?
  • Grieger and Marsden used an experiment suggested
    by Ernst Rutherford, a premier physicist and
    often considered the Faraday of nuclear physics.
  • The experiment consisted of using gold tin foil
    about 400 atoms thick with He particles as
    their bombarding projectiles.
  • Most of the particles went straight through with
    no deflection, which seemed to support classical
    theory, since it is known that electrons are much
    smaller and thus when all charge is equally
    distributed, there would be little deflection
  • HOWEVER, this was not the case for all particle,
    there were a given number that were scattered
    back at angles larger than 90 degrees, implying
    something else is going on.
  • Rutherford, examined the results and concluded
    that the bulk of the atom and the majority of
    positive charge, HAD to be concentrated at a
    single point in the atom.

15
  • Thus, the concept of a nuclear atom model was
    presented. However, this causes more problems.
  • With this model, under classical theory, it would
    necessarily yield a continuous spectrum, since
    there is no partitioning of the energy, thus no
    constraints on either the frequency or
    wavelength.
  • With classical theory again failing to explain
    the observed phenomena, physicist began searching
    for an explanation and theory that accurately
    describes reality.

16
Now that we know the problems let fix them!
Lets meet the mechanics
  • The Big Wigs
  • -Max Plank
  • -Niels Bohr
  • -Albert Einstein
  • -de Broglie
  • Other notable participants (Max Born, John von
    Neumann, Paul Dirac)

17
Who is Max Plank??
  • Brief Background
  • Planck came from traditionally intellectual
    background, his great grandfather and grandfather
    were both theology professors, while his father
    was a law professor and uncle was a judge
  • He studied under Hermann Muller at Munichs
    Königliches Maximiliangymnasium, where he was
    taught mechanics, astronomy, and mathematics
  • An incredibly gifted child, he graduated at the
    age of 16 and in 1874 began studying at
    university of Munich

18
Background Continued
  • While at university, he was advised by his
    professors not to study physics, because they
    believed that nearly everything had already been
    discovered and all that was left to do was fill
    in a few holes
  • However, this did not discourage Planck, rather
    he claimed that he was not in the field to make
    revolutionary discoveries, but rather to gain a
    fuller understanding of those theories already
    established
  • This desire for complete understanding,
    consequently led him to arguably, one of the
    greatest discoveries in modern physics, since he
    refused to accept that classical theory just
    didnt explain reality.

19
Career background
  • Planck did very few experiments before entering
    into the realm of theoretical physics. He was
    more concerned with why things were happening,
    than searching for new observational realities
  • He went to Berlin to study with two of the
    premiere physicists of the time, Hermann von
    Helmholtz and Kirchhoff
  • Studying entropy and thermodynamics, he was
    eventually appointed to the position of
    Kirchhoffs successor
  • These events gave him the background needed to
    make his revolutionary discoveries

20
What exactly were Plancks findings??
  • Planck worked on the Blackbody radiation problem
  • Plank was hired by electrical companies to find a
    way to produce the most light (radiation) using
    the least amount of energy possible.
  • Since he had worked under Kirchhoff, Planck new
    that Kirchhoff had already contemplated the
    question of how the intensity of the radiation
    emitted by a blackbody depends on the frequency
    of the radiation
  • Thus, Planck decided to utilize a collection of
    radiating harmonic oscillators in thermal
    equilibrium to describe black body radiation

21
Quick Review
  • We know that classical methods had failed to
    describe the observational reality as seen
    through its discrepancy with the Ryleigh Jean
    equation, since it failed to work for short
    wavelengths.
  • There was also conjecture presented by Willheim
    Weil that described the phenomena for short
    wavelengths, but failed for long wavelengths.
    Thus Planck decided to utilize both ideas and
    interpolate between the two.

22
  • To do this, Planck used a thermo dynamical
    argument to produce a two parameter ad hoc
    expression which we will see later.
  • He did this through modification of classical
    relations involving entropy of radiation
  • His argument was incredibly complex, and too
    intense to derive currently, however, it is
    imperative to note that it was incredibly based
    on phenomological curve fitting
  • Basically, he was left with a curve that fit the
    observed data perfectly, but had no solid
    theoretical justification for his results.

23
Why Why Why
  • Thus, he returned to his studies in order to try
    to derive a theoretical justification
  • To do this, he found that he was required to
    utilize statistical mechanical techniques
    (which allows for distributions to be describe on
    its micro state) which had been introduced by
    Boltzmann.
  • This was a big step, because he had been
    extremely reluctant to accept these new
    techniques, because he felt they were merely
    axiomatic by nature
  • However, he claimed it was an act of despair I
    was ready to sacrifice any of my previous
    convictions about physics.

24
  • Though he was originally reluctant, he allowed
    himself to accept these new techniques, which
    allowed him to partition the total energy of the
    system into discrete amounts
  • Therefore, his oscillators could only absorb and
    emit discrete amounts of radiation which
    consequently yielded the proper distribution.
  • Through these methods, he arrived at the notion
    that the energy absorption and emission must be
    quantized into discrete amounts e (modernly
    referred to as quanta)

25
Final result!! ?
  • Thus, Planck had a theoretical basis and
    therefore showed that the energy e , is related
    to the frequency v by
  • e hv. where h is Plancks constant

26
Still Hesitant
  • Though he was certain that energy absorption and
    emission had to be quantized, and was described
    by the formula, he was still hesitant to accept
    energy quantization in electromagnetic radiation.
  • He felt that Maxwells electrodynamics, which
    claimed that an electromagnetic field could carry
    continuously varying amounts of energy, had been
    too successful to just disregard them
  • He spent much time trying to fit his prior
    finding of e hv. into classical
    electrodynamics, however, after many failed
    attempts, he came to a final conclusion accepting
    the reality of quanta, which has since been
    accepted by nearly all physicists.
  • This is evident today, as we readily use the
    notion of a photon, which is merely the name for
    a quantized electromagnetic field.

27
So What?
  • How does this solve the problem which arises from
    classical mechanics??
  • Look at the equation for wavelength
  • v c / ?
  • we see that Plancks equation e hv hc / ?
  • Thus, if energy is finite, there must exist a
    shortest and a longest wavelength, and thus, if
    very few quanta are released when ? is either
    large or small.
  • Further, it is obvious from the equation that the
    peak will occur at the most probable frequency.

28
Mile Marker 1
  • With Plancks recognition that energy could in
    fact be discretely quantized, an entire new wave
    of physical thought arose
  • Plancks findings are often considered the birth
    of quantum mechanics.
  • However, this is merely the first step lets now
    look to the problem of discrete emission of
    spectral lines.

29
AN ATOMIC TRANSMISSION (uh transition)!Niels Bohr
  • Who is Niels Bohr?
  • Bohr made many notable contributions to physics,
    namely
  • A model of the atomic structure
  • Electron orbital momentum is quantized by Lnh
  • Notion that electrons travel in discrete orbitals
  • Notion that when electrons drop from higher to
    lower energy, it emits a photon
  • The principle of complementarity

30
Why we need him
  • Though he made notable contributions, we will
    focus on his theory of atomic transitions
  • Bohr attended the University of Copenhagen and
    then went to Manchester to work under Rutherford,
    who (as we saw previously) was actively working
    on developing an atomic model
  • This influenced Bohr greatly, and within four
    months of working with Rutherford, he formulated
    his theory.

31
Lets Derive the Theory
  • Bohr began by assuming Rutherfords model, ie an
    electron of charge e and mass m in circular
    orbit of radius r about the nucleus (charge e)
  • Thus, if a stable nuclear orbit is to be
    attained, the electrostatic force of attraction
    must yield the imperative centripetal force.

32
Where is this going?
  • Knowing this, and applying the law of
    conservation of energy, Bohr derived the
    following expression
  • which represents the frequency in relation to its
    energy.
  • However, if we were to apply classical theory
    (which implies that an accelerated particle emits
    radiation wit frequency equal to that as seen
    above) problems obviously arise.

33
Whats Wrong?
  • According to classical theory, the energy E could
    be of any value and thus the atom should radiate
    all frequencies, yielding a continuous spectrum.
    However, we know this is not the case as seen
    prior
  • Therefore, Bohr began working to attain a set of
    discrete orbits such that it is stable only when
    the electron is within one the these distinct
    orbitals, and thus only emits radiation when
    transitioning between them.

34
Follow the Leader
  • Knowing that Planck had quantized energy emitted
    and absorbed in oscillators, Bohr decided to
    quantize the energy of the photons released when
    entering and leaving the stable orbits.
  • With this concept, he derived the equation
  • He introduces the factor of ½ because if the the
    electron is initially at rest and its final state
    is in the stable orbit, then it will have
    velocity v, thus the average between the two is
    simply v/2.
  • However, it must be noted that he did not come
    up with this justification until he examined
    Balmers equation (presented earlier) and found
    that it was the ½ factor that allowed for an
    accurate fit)

35
  • Therefore, he felt that the emitted radiation
    would be some multiple of this, which led to the
    n/2 factor.
  • By combining this derivation with the expression
    of frequency in terms of energy, Bohr obtained
    the expression
  • Further, when combined with the conservation of
    energy law E(final) E(initial) hv, Balmers
    equation is obtained, and thus, the spectral
    lines emitted by Hydrogen are accurately depicted
    by Bohrs expression.

36
Even Better!
  • Bohr also stated that using the same techniques
    and theory, his derived expression, was
    equivalent to quantizing angular momentum l
    mvr.
  • This is very efficient, but similar to past
    explanations, thus we will not derive here.

37
Does it Work?
  • Bohrs model works quantitatively for
    one-electron atoms such as hydrogen, ionized
    helium, and doubly ionized Lithium.
  • Though his original model only worked for these
    few elements, his work made immediate impact and
    commanded much attention.
  • After he presented his work in 1913, many
    generalizations were made and a set of rules for
    treating atoms was establishes (modernly referred
    to as old quantum theory)

38
How we go from one to another
  • A three step process was employed to move from
    classical to quantum theory when describing
    atomic structure
  • Initially, classical theory is used to determine
    the possible motions of the system
  • Secondly, quantum theory is employed to depict
    the possible orbits
  • And finally, the law of energy conservation is
    employed to fix the frequencies during an atomic
    transition

39
Who Cares?
  • Does it really matter how Bohr arrived at his
    model of the atom, or how Bohr determined that
    the frequency of an atom depends on the negative
    of its energy raised to the 3/2 power?
  • Does anyone need to know this besides scientific
    historians and PHIL/PHYS 30389 students?
  • Probably not
  • However, insight into the process helps make the
    discoveries more understandable

40
Brilliance or Backpedaling?
  • We see Plank makes an ad hoc attempt to make some
    argument to justify his curve fitting
  • Then, against his will, he accepts the hypothesis
    of quantization
  • Energy quantization providing the necessary
    limitation on the blackbody radiation curve at
    short wavelengths was not a moment of brilliance
    but instead a drawn out process Plank himself
    wanted to avoid

41
Brilliance or Backpedaling 2?
  • Bohr in a desperate panic to obtain a fit to the
    data (our good friend the Balmer formula)
  • By 1913 Planks quantization of energy is highly
    accepted so Bohr is not as adamant about avoiding
    it
  • Bohr is conservative in his methods, for example
    sought to quantize energy and not angular
    momentum
  • His attempts to avoid numerous new principles
    leads to the acceptance of his theory
  • Dont you appreciate their work better now???

42
Fork in the Road
  • At this point in history the theory of
    indeterminism was a serious question for the
    enlightened
  • Poincare, Høffding, and Kierkegaard all
    incorporated quantum theory into their work
  • Høffding claimed that decisive events in life
    proceed through discontinuities, or sudden
    jerks, which faintly resembles atomic phenomena
  • These ideas were in the minds of scientists,
    which helps explain why some were more inclined
    to accept certain models of quantum theory

43
Team New School, turn left
  • Bohr, Heisenberg, Pauli, Jordon, and Born
  • All found in Copenhagen
  • Exclusive group who worked together and rarely
    sought help from others
  • New School were inclined towards a discontinuous
    structure in nature at the most fundamental level
    and to a doctrine of complementary between
    opposites
  • Discontinuousness was the language used by these
    men to describe atomic phenomena
  • NOTE Causality was not the central question in
    the development of the theory

44
New School does Philosophy
  • Because of the failures of some classical
    approaches team New School took up new
    philosophical positions on what was possible
  • Bohr believed the failure of the classical
    mechanics explaining the electron theory of
    metals was due to an insufficiency in the
    classical principles
  • Pauli was convinced that a Continuum Field
    theory, with particles as singularities, was not
    possible
  • Pauli and Heisenberg decided electron orbitals
    were meaningless because of the failure to apply
    old quantum theory to molecular systems
  • There existed a clear desire to revolutionize the
    concepts of the time

45
  • From 1924-1927 Heisenberg worked on his version
    of the quantum model
  • Of note are his operators, which have the
    unusual property that the order of multiplication
    matters (AB?BA usually)
  • We now know this is usually the case when A and B
    are (n x n) matrices, ngt1, and is standard
    matrix multiplication
  • The new math seemed mysterious yet worked
    extremely well, seemed promising.and for real
    there were no other alternatives
  • This new math is discrete (as opposed to
    continuous) which appealed to and suited well New
    Schools understanding of the nature of the atom

46
Team Old School, turn right
  • Einstein, Louis de Broglie, and Schrodinger
  • Not as closed at Team New School
  • Considered the continuous wave as the basic
    physical entity subject to a causal description
  • Team Old School avoids the notion of
    discontinuity and other radical ideasmaking them
    team Old School

47
Einsteins influence
  • Einstein views the foundational questions of
    physics (such as relativity, quantum theory,
    unified field theory) as the search for a
    rational, causal reasoning which can be
    comprehended in terms of objective realitywhich
    suggests a continuity of basic physical processes
  • In 1909 Einstein used Blackbody radiation to
    show the radiation exhibited wave and particle
    behaviors
  • However after showing that the direction a
    molecule has after emitting radiation is left to
    chance, Einstein proclaimed it a mistake of the
    theory

48
De Broglie
  • In 1923 he started the theory of wave mechanics
    to try to understand the dual nature of a photon
  • Interested in the dual nature of light, proposed
    a model of a particle that followed the
    trajectory determined by its associated waves
  • De Broglie turned mathematical analogy between
    waves and particles into theory
  • Later Schrödinger gave a plausibility argument
    for his wave equation

49
Review
  • New School
  • From Copenhagen school
  • Discontinuous school
  • Saw need to revolutionize current principles
  • Old School
  • Not From Copenhagen school
  • Continuous school
  • Committed to continuous wave as basic physical
    entity subject to causal description

50
Fight!
  • The 2 quantum theories did not coexist long
  • Their collision lead to the eventual consistent
    interpretation of quantum mechanics
  • We will now see how the Copenhagen (Old School)
    interpretation established dominance over all
    other lesser versions of quantum theory

51
Philosophy actual effects something!
  • Old school is from an older generation which is
    less likely to accept philosophical ideas such as
    indeterminism and randomness in nature
  • New School more willing to accept radical
    theories, such as indeterminism and unusual
    atomic motions

52
Subatomic Kombat
  • Heisenbergs Matrix mechanics had no physical
    interpretation, but worked quitewell.
  • Heisenberg thought classical mechanics could not
    be changed in order to make sense of quantum
    phenomena without destroying the theory, hence
    the need for a new theory
  • Heisenberg bothered by Schrödinger unique
    formalism concerned with continuous,causal,
    visible properties
  • But it turns out

53
Matrix Mechanics and Wave Mechanics Formalisms
are Mathematically Equivalent!
54
The Race is On
  • There became a great push to determine the
    correct interpretation of Matrix Mechanics
  • For calculation purposes many scientist were
    adopting the Wave-Mechanics model
  • Heisenberg had personal ambitions and could not
    let Old School steal his subatomic thunder
  • For the love of god the fate of the direction of
    theoretical physics was at stake!!!

55
  • New School worked together in Copenhagen as a
    team to push the matrix mechanics model
  • Heisenbergs uncertainty principle helped
    establish New School as the leading school of
    quantum thought
  • Meanwhile Old School is doing their own thing
    working on individual projects
  • Thus Copenhagen is able to take charge and
    influence a centurys worth of thought

56
  • At the 1927 Slovay Congress, de Broglie suggested
    a synthesis of the wave andparticle nature of
    matter.
  • Pauli used a specific example to criticize de
    Broglies theory de Broglie and others responded
    poorly or not at all, leaving the Copenhagen
    theory to be accepted.
  • Experience has shown the consistency of the
    Copenhagen interpretation and that fundamental
    atomic phenomena are discrete
  • Physical reality is whatever quantum mechanics
    is capable of describing Cushing on Borhs
    thoughts
  • The subjective epistemological criterion of the
    need for classical concepts to describe the
    results of measurements Cushing on Copenhagens
    thoughts

57
  • Copenhagen interpretation refers to a common set
    of principles shared by a group of scientists who
    follow Bohr.
  • Differences between Old School should be clear
  • New School was by no means in total agreement
    over quantum theory
  • The next presentation will explain this!!

58
Works Cited
  • Wikipedia- The Free Encyclopedia
  • Philosophical Concepts In Physics James Cushing
  • From X-Rays to Quarks Emilio Segré
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