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29 September 2017 ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg The isolated electron: De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed BPS Monopole International Conference on Numerical Analysis and Applied Mathematics 2017, Thessaloniki R. Hofmann, Institut für Theoretische Physik, Universität Heidelberg
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Page 1: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

29 September 2017

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

The isolated electron: De Broglie's „hidden“ Thermodynamics,

SU(2) Quantum Yang-Mills theory, and a strongly perturbed BPS Monopole

International Conference on Numerical Analysis and Applied Mathematics 2017, Thessaloniki

R. Hofmann, Institut für Theoretische Physik, Universität Heidelberg

Page 2: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

outline

Louis de Broglie's arguments on existence of „thermodynamics of the isolated electron“

Page 3: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

outline

Louis de Broglie's arguments on existence of „thermodynamics of the isolated electron“

phase diagram of SU(2) Quantum Yang-Mills thermodynamics - deconfining, preconfining, and confining phases - thermal ground state and its excitations in deconfining phase - center-vortex loops in confining phase

Page 4: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

outline

Louis de Broglie's arguments on existence of „thermodynamics of the isolated electron“

phase diagram of SU(2) Quantum Yang-Mills thermodynamics - deconfining, preconfining, and confining phases - thermal ground state and its excitations in deconfining phase - center-vortex loops in confining phase

electric-magnetically dual interpretation of U(1) charges in SU(2) YMTD

- value of coupling , caloron action - finestructure constant → dual interpretation of

Page 5: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

outline

Louis de Broglie's arguments on existence of „thermodynamics of the isolated electron“

phase diagram of SU(2) Quantum Yang-Mills thermodynamics - deconfining, preconfining, and confining phases - thermal ground state and its excitations in deconfining phase - center-vortex loops in confining phase

electric-magnetically dual interpretation of U(1) charges in SU(2) YMTD

- value of coupling , caloron action - finestructure constant → dual interpretation of

strongly perturbed BPS monopole

- expanding spherical shells - breathing mode of monopole core

Page 6: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

outline

Louis de Broglie's arguments on existence of „thermodynamics of the isolated electron“

phase diagram of SU(2) Quantum Yang-Mills thermodynamics - deconfining, preconfining, and confining phases - thermal ground state and its excitations in deconfining phase - center-vortex loops in confining phase

electric-magnetically dual interpretation of U(1) charges in SU(2) YMTD

- value of coupling , caloron action - finestructure constant → dual interpretation of

strongly perturbed BPS monopole

- expanding spherical shells - breathing mode of monopole core

electron as self-intersecting, spatial center-vortex loop: size estimates

Page 7: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

Louis de Broglie: reminder of derivation of wavelength , I

- consider particle at rest as a `clock´ with frequency which extents through a large portion of space, that is, amplitude of oscillation is the same everywhere:

- by the rules of QM: rest energy equals quantum of action times :

- consider Lorentz-trafo in direction:

spatially “flat” oscillation becomes propagating wave with

Page 8: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

Louis de Broglie: reminder of derivation of wavelength , II

- on the other hand:

or upon substitution of

-

existence of `clock´ frequency essential in derivation of

de Broglie wavelength !

Page 9: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

Thermodynamics of isolated electron: Louis de Broglie

- from demand that entropy

is a fundamental invariant under the Poincare group and from

(considering an adiabatic variation of rest mass due to input of heat)

- increase of rest energy under boost can be decomposed into a decrease of internal heat to

and work invested to boost the particle

Page 10: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

Thermodynamics of isolated electron: Louis de Broglie

Particle with internal heat

can not be point-like.

How does SU(2) Yang-Mills thermodynamics

come in?

Page 11: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

Phase diagram of SU(2) Quantum Yang-Mills thermodynamics

deconfining preconfining confining

Hagedorn 2nd order

coupling

Page 12: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

Phase diagram of SU(2) Quantum Yang-Mills thermodynamics:Confining phase

excitations: n-fold self-intersecting center-vortex loops

stable

unstable

multiplicity [Bender & Wu, 1969]

Page 13: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

Proposal for electron's anatomy

(i) electric-magnetically dual interpretation of U(1) charges in SU(2)

(ii) classical dynamics of strongly perturbed BPS monopole [Fodor & Racz, 2004]

(iii) structure of deconfining thermal ground state, small-holonomy (anti)calorons, dissociation of large-holonomy (anti)calorons [Herbst & RH, 2004; RH, TQYM,2016]

based on:

Page 14: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

(i) electric-magnetically dual interpretation: deconfining-phase gauge coupling and caloron action

thermodynamical consistency

small-mass expansion, pressure[Dolan et Jackiw (1974)]

transition to preconfining phase

SU(3)

SU(2)

Page 15: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

thermodynamical consistency

small-mass expansion, pressure[Dolan et Jackiw (1974)]

transition to preconfining phase

SU(3)

SU(2)

- restore

coarse-graining dominated by

[Brodsky et al. (2011); Kaviani & RH 2012;RH 2012,2013]

(i) electric-magnetically dual interpretation: deconfining-phase gauge coupling and caloron action

Page 16: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

if SU(2) something to do with photons [RH (2005), Grandou & RH (2015), etc] then electric-magnetically dual interpretation required: in units fine-structure constant

(i) electric-magnetically dual interpretation: argument involving QED fine-structure constant

Page 17: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

if SU(2) something to do with photons [RH (2005), Grandou & RH (2015), etc] then electric-magnetically dual interpretation required: in units fine-structure constant

(i) electric-magnetically dual interpretation: argument involving QED fine-structure constant

Page 18: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

if SU(2) something to do with photons [RH (2005), Grandou & RH (2015), etc] then electric-magnetically dual interpretation required: in units fine-structure constant

for to be unitless:

( )

(i) electric-magnetically dual interpretation: argument involving QED fine-structure constant

Page 19: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

if SU(2) something to do with photons [RH (2005), Grandou & RH (2015), etc] then electric-magnetically dual interpretation required: in units fine-structure constant

for to be unitless:

But: magnetic coupling in SU(2)

SU(2) to be interpreted in an electric-magnetically dual way. (e.g., magnetic monopole electric monopole, etc.)

( )

(i) electric-magnetically dual interpretation: argument involving QED fine-structure constant

Page 20: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

(ii) classical dynamics of strongly perturbed BPS monopole

- hyperboloidal conformal transformation of the original field equations for the profiles

and

of the adjoint Higgs and off-Cartan gauge fields fields, respectively

- under a spherically symmetric initial pulse in energy density: - high-frequency oscillations in forming expanding shells

[Fodor & Racz, 2004]

Page 21: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

(ii) classical dynamics of strongly perturbed BPS monopole

- a localized breathing state appears in association with the energy density within the monopole core whose frequency approaches the mass

of the two off-Cartan modes in a power-like way in time

[Fodor & Racz, 2004]

Page 22: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

(ii) classical dynamics of strongly perturbed BPS monopole

There is a generic circular frequency

associated with core breathing of the (initially perturbed) BPS monopole, that is, a clock in de Broglie's sense.

Page 23: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

(iii) structure of deconfining thermal ground state

- If monopole liberated by dissociation of a large-holonomy caloron in deconfining phase at temperature then

[Diakonov et al 2004]

- Only (anti)calorons of scale contribute to emergent a priori estimate of thermal ground state coupling relevant in describing caloron dissociation and ensuing monopole- antimonopole

[Herbst & RH 2004; RH 2016]

Page 24: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

(iii) structure of deconfining thermal ground state

[Diakonov et al 2004]We have:

(A)

(B)

with:

We assume static BPS monopole of mass

to be immersed into blob of deconfining phase of radius at .

Page 25: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

Size estimate for self-intersection region:

[RH, 2017]

Thus, from (A) and (B) we have:

Comparing this to the Compton wave length m,

(~ 4.12 core size of monopole)

Page 26: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

hierarchy between Yang-Mills scale (~ ) and electron mass and Coulomb self-energy:

from

eV

For comparison: average electron temperature at ITER envisaged to be

eV !!

Coulomb self-energy correction:

Page 27: The isolated electron: De Broglie's „hidden“ Thermodynamics ...hofmann/R_Hofmann...De Broglie's „hidden“ Thermodynamics, SU(2) Quantum Yang-Mills theory, and a strongly perturbed

ICNAAM 2017 R. Hofmann, ITP, Uni Heidelberg

Summary and outlook ● brief review of Louis de Broglie's argument on electron's inherent

thermodynamics

● phase structure of SU(2) YMTD, deconfining phase, confining phase

● electron as a one-fold self-intersecting center-vortex loop

● strongly perturbed BPS monopole

● structure of deconfining thermal ground state

● size estimates

● Coulomb self-energy and relation between Yang-Mills scale and crit. Temp.

● open questions: - spherically symmetric perturbation of BPS monopole generalizable to other perturbations - spatial extent of loops (depending on environmentally provided resolution?) - Schrödinger wave mechanics facilitated by small core sizes vs. - What happens under acceleration? (radiation, radiation reaction,...)


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