photon time delay due to the presence of a magnetic...
TRANSCRIPT
Photon time delay due to the
presence of a magnetic field.
Varadero, Cuba 2018
MsC. Lidice Cruz Rodríguez
Dra. Aurora Pérez Martínez
Dra. Elizabeth Rodríguez Querts
Dr. Jorge Rueda
Physics Faculty, Havana University
ICIMAF
ICRANet, Pescara, Italy
Outline Outline
Motivation.
Propagation of photons in a magnetic field:
Dispersion equation in the vacuum
Dispersion equation in the medium
Phase velocity, preliminary results.
Some remarks and future work directions…..
Outline Motivation
It is known how the interaction with the
medium delay the photon propagation.
Higher energy photons arrive before.
How the propagation in the magnetosphere
affects the photon dispersion law and hence
the photon velocity?
Delay in photon propagation is used to
measure pulsars distance!
Polarization tensor, theoretical overview.
In the presence of an external magnetic field B along the 𝑥3 direction the
diagonalization of the polarization tensor leads to the equation:
Having three non vanishing eigenvalues
and three eigenvectors for i=(1,2,3),
corresponding to the three photon
propagation modes
Π𝜇𝜈𝑎𝜈(𝑖)= 𝜅(𝑖)𝑎𝜇
(𝑖)
𝑎𝜇(1)= 𝑘2𝐹𝜇𝜆
2 𝑘𝜆 − 𝑘𝜇 𝑘𝐹2𝑘
𝑎𝜇(2)= 𝐹𝜇𝜆∗ 𝑘𝜆
𝑎𝜇(3)= 𝐹𝜇𝜆∗ 𝑘𝜆
𝑘2 = 𝑘⊥2 + 𝑘∥
2 − 𝜔2
For 𝐤 ⊥ 𝐁 𝐚𝛍𝟏
is a longitudinal and non
physical mode, 𝐚𝛍𝟐,𝟑
are transverse modes.
For 𝐤 ∥ 𝐁, 𝐚𝛍𝟐
is a longitudinal and non
physical mode, 𝐚𝛍𝟏,𝟑
are transverse modes,
Which leads to circular polarized waves
(Faraday effect).
Quantum Faraday EffectDispersion equation
𝑘2 = 𝜅(𝑖)(𝑘2, B)The dispersion equation is then
Eigenvalues of the polarization tensor
From the solution of the dispersion equation the information related to
photon propagation can be obtained.
Quantum Faraday EffectDispersion equation
𝑘2 = 𝜅(𝑖)(𝑘2, B)The dispersion equation is then
Eigenvalues of the polarization tensor
From the solution of the dispersion equation the information related to
photon propagation can be obtained.
Here we will solve the dispersion equation in two particular cases and we
will show preliminary results for the phase velocity.
Quantum Faraday EffectDispersion equation
𝑘2 = 𝜅(𝑖)(𝑘2, B)The dispersion equation is then
Eigenvalues of the polarization tensor
From the solution of the dispersion equation the information related to
photon propagation can be obtained.
Here we will solve the dispersion equation in two particular cases and we
will show preliminary results for the phase velocity.
Photon propagation in the vacuum in the presence of an external magnetic field.
Photon propagation in the medium in the presence of an external magnetic field.
Quantum Faraday EffectPhoton propagation in the vacuum
In general the renormalized eigenvalues of the polarization tensor in the one
loop approximation can be written as
In the range of frequencies with small deviation from the light cone 𝑘2
𝑒𝐵≪ 1
𝜅𝑖(𝑘2, 𝐵) =
2𝛼
𝜋
0
∞
𝑑𝑡
−1
1
𝑑𝜂 𝑒−𝑡𝑏 𝜌𝑖𝑒
𝜁 +𝑘2 𝜂2
2𝑡
𝑓(𝑘2, 𝐵)
𝝌𝒊𝒍 =2𝛼
𝜋
0
∞
𝑑𝑡
−1
1
𝑑𝜂 𝑒−𝑡𝑏 𝑒𝜁0
𝜍
𝑏𝑚2
𝑙 (−1)𝑙
𝑙!𝜌0𝑖 − 𝑙
𝜍
𝑏𝑚2
−1
𝜃𝑖 + 𝛿1𝑙 𝜂2
2𝑡
𝜿𝒊 𝑘2, 𝐵 =
𝑙=0
∞
𝝌𝒊𝒍 (𝒌𝟐)𝒍≈
𝑙=0
𝑛
𝜒𝑖𝑙 (𝑘2)𝑙
Quantum Faraday EffectPhoton propagation in the vacuum
𝜿𝒊 𝑘2, 𝐵 = 𝑘2 ≈
𝑙=0
𝑛
𝜒𝑖𝑙 (𝑘2)𝑙
𝑘2 = −
𝑗2,𝑗3…𝑗𝑛≥𝑛
(−1)𝑗1𝑗1!
(𝑗0+1)! 𝑗2! 𝑗3! … 𝑗𝑛!
𝜒𝑖0𝑗0+1𝜒𝑖2
𝑗2𝜒𝑖3𝑗3 …𝜒𝑖𝑛
𝑗𝑛
(𝜒𝑖1 −1)𝑗1+1
i=2,3
𝒌⊥(𝟐,𝟑)≈ 𝝎𝟐 + 𝒌(𝝎,𝑩)𝟐
𝒗(𝑩,𝝎) =𝝎
𝒌⊥(𝝎,𝑩)
As we can see the phase velocity in general depends on the magnetic field B
and the photon energy.
Quantum Faraday EffectResults
Dispersion equation Phase velocity
ℏ𝜔2
𝑚2
𝑘⊥2/𝑚2
ℏ𝜔 2
𝑚2
𝑣(𝑚/𝑠)
Quantum Faraday EffectPhoton propagation in the medium, diluted gas limit
𝒗(𝑩,𝝎) =𝝎
𝒌⊥(𝝎,𝑩)
Dispersion equation
𝑘2 = 𝜅(𝑖)(𝑘2, 𝜇, B)
𝑘∥(1,3)≈ 𝜔2 + 𝑘(𝜔, 𝐵)2
We have different 𝜅(𝑖) .
Solution for the particular case of 𝐤 ∥ 𝐁.
Diluted gas limit
(classical distribution of particles)
𝑘∥(1,3)≈ − 𝑒𝐵 ±𝑚𝜔 + 2𝑒𝐵 ± 2𝑚𝜔2 − 2𝐴 𝐵, 𝑇, 𝜇 𝑚𝑤
1/2
Phase velocity 𝑣(𝐵,𝜔) =𝜔
𝑘∥(𝜔, 𝐵)
Quantum Faraday EffectResults
𝒗(𝑩,𝝎) =𝝎
𝒌⊥(𝝎,𝑩)
Phase velocity
𝑣(𝑚/𝑠)
ℏ𝜔/𝑚
Photon time delay
ℏ𝜔(𝑒𝑉)
Δ𝑡(𝜇𝑠)
The time delay between radio
frequency photons and micro wave
frequency photons is around 0.7𝜇𝑠
Some remarks
We have solved the dispersion equation in two limit cases, for propagation in
a magnetized vacuum perpendicular to the direction of the constant magnetic
field, and in a medium in the diluted gas limit.
We show the dependence of the phase velocity with the photon energy,
for propagation in the vacuum we found that the higher energy photons are
delay with respect to the lower energy ones.
In the medium (under the limits considered) the higher energy photons
travels faster.
What is coming next…..
ArXiv:gr-qc/9503044v1 25 Mar 1995
Include a more realistic model for the
magnetic field of a rotating neutron star,
dipolar approximation
Combine calculations to describe the
different regions traversed by the
radiation coming from the pulsar.
Estimate delay times and compare with
experimental data which is available.
Varadero, Cuba 2018
Gracias!!!!