DAMPING THE FLAVOR PENDULUM BY BREAKING HOMOGENEITY (Alessandro MIRIZZI, Hamburg U.)
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Transcript of DAMPING THE FLAVOR PENDULUM BY BREAKING HOMOGENEITY (Alessandro MIRIZZI, Hamburg U.)
DAMPING THE FLAVOR PENDULUMDAMPING THE FLAVOR PENDULUMBY BREAKING HOMOGENEITYBY BREAKING HOMOGENEITY
(Alessandro MIRIZZI, Hamburg U.)(Alessandro MIRIZZI, Hamburg U.)
NOW 2014NOW 2014Neutrino oscillation workshopNeutrino oscillation workshop
Conca Specchiulla, 07-14 September 2014Conca Specchiulla, 07-14 September 2014
(Based on work in collaboration with G. Mangano & N. Saviano, (Based on work in collaboration with G. Mangano & N. Saviano, 1403.1892)1403.1892)
*
*
e
e
eeee
DENSITY MATRIX FOR THE NEUTRINO ENSEMBLE
Diagonal elements related to flavor content
Off-diagonal elements responsible for flavor conversions
),(
),(
rEF
rEF
In 2scenario. Decompose density matrix over Pauli matrices to get the “polarization” (Bloch) vector P. Survival probability Pee =1/2(1+Pz) . Pz = -1 -> Pee =0 ; Pz = 0 -> Pee =1/2 (flavor decoherence)
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
EQUATIONS OF MOTION FOR A DENSE NEUTRINO GAS
],[ ,,,,, xpxpxppxpxpxpt ipv
(Sigl & Raffelt, 1992)
Liouville operator Hamiltonian
xpt , Explicit time evolution
xpxpv , Drift term due to space inhomogeneities
xppp , Force term acting on neutrinos (negligible)
7-dimensional problem. Never solved in its complete form. Symmetries have been used to reduce the complexity of the problem.
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
mattvacxp,
SPACE/TIME HOMOGENEITIY
Space Homogeneity:
],[ ,,,, xpxpxpxpxpt iv
Pure temporal evolution (Neutrinos in Early Universe)
Time Homogeneity:
],[ ,,,, xpxpxpxpxpt iv
Stationary space evolution (SN neutrinos)
However, small deviations from these symmetries have to be expected. Can these act as seed for new instabilities?
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
TOY MODEL: PENDULUM IN FLAVOR SPACE
PDLBP
PDLBP
t
t
][
][
PPD
)1(2
1 Pp Two-flavor polarization vectors
E
m
2
2 Vacuum oscillation frequency
eFnG2 Matter potential. Large HOMOGENEOUS can be rotated away !
nGF2 potential
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
FLAVOR OSCILLATIONS AS SPIN PRECESSION
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
Slide from G. Raffelt
HOMOGENEOUS PENDULUM
Periodic pair conversions in IHxxee
((
For homogeneous
[Hannestad et al, astro-ph/0608695]
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
,e e
,
NON-HOMOGENEOUS BACKGROUNDS
),()],(),(),([),()( txPtxDtxLtxBtxPtx
The partial differential equation can be transformed into a tower of ordinary differential equations for the Fourier modes
ikxk etxdxPtP ),()(
)],([)(
)],([)(
txFTt
txFTt
k
k
(1D spatial motion)
MONOCHROMATIC MATTER INHOMOGENEITY
)cos( 0xk )]()([ 00 kkkkk FT
const )(2 kk
0nkkn
nkn PP
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
EOMs for the n=0,1 modes
Starting from homogeneous initial condition: only 00 P , n ≥ 1 modes are excited in sequence
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
DAMPING THE FLAVOR PENDULUM
310
0
710
A small seed of inhomogeneity is enough to produce a run-away from the stable pendulum behavior. The average P0 tends towards the flavor equilibrium.
20 k pendulum oscillation frequency
1403.1892
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
TRAJECTORIES OF THE FLAVOR PENDULUM
((
0 310
Stable pendulum Unstable pendulum
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
EVOLUTION OF DIFFERENT FOURIER MODES
310
n=1
n=2
n=3 n=4
After P1 starts rising, the higher Fourier modes are also rapidly excited in sequence reaching | Pn|~0.1
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
DEPENDENCE ON PERTURBATION WAVE-NUMBER
ck 0
1c
210c
210c
1c The flavor decoherence is approached earlierkk 0
210c Longer perturbation wave-length. The system needs more cycles to feel inhomogeneities210c Perturbations are averaged during an oscillation cycle. The effect is shifted al later timesAlessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
NON-TRIVIAL SPACE BEHAVIOR
ikxk etdkPtxP )(),(
homogeneous solution
inhomogeneous solutions
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
DECLINING NEUTRINO DENSITY
)/exp(0 t
Quick decoherence. Similar to the case of constant
Lowering the system requires more time to decohere. Decoherece is not complete.
For a too fast decline, the system has not enough time to decohere
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014
CONCLUSIONS
We studied the effects of small inhomogeneities on the self-induced evolution of a dense neutrino gas, by Fourier transforming the EOMs
We found that the neutrino flavor pendulum is not stable under the effects of small inhomogeneities
However, a declining neutrino potential can suppress the effect of the inhomogeneities
The effect on the flavor evolutions of neutrinos in SN or in the Early Universe needs further investigations with more realistic models.
Alessandro Mirizzi NOW 2014 Conca Specchiulla, 8 September 2014