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A Prime-Index Estimate of Neutrino-Nucleon Cross Sections
Ali R. Fazely
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Outline
What is a Neutrino?
How to Calculate 𝝂-N Cross Section Using Q.M.?
Prime-Index Estimate
Conclusions and Open Questions
Ali R. Fazely, Miami Conference, December 16 -22, 2015
What is a Neutrino?• An elementary particle, not part of
ordinary matter
• No electric charge, ½ integer spin, very little mass
• First postulated by Pauli (1930) to explain beta-decay
• Lepton Family:
– e-, Electon Neutrino 𝝂e
– µ, Muon Neutrino 𝝂µ
– τ, Tau Neutrino 𝝂τ
• Possesses only weak interaction and gravity
• There are lots of them!
Beta Decay
of a Neutron
n
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Neutrinos within the Standard Model
https://simple.wikipedia.org/wiki/Elementary_particle
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Where do Neutrinos come from?
Source of ’s
Nuclear Reactors
few MeV
Human Body
= 3.4 x 108/day
Earth’s Radioactivity
6 x 106/cm2s
Accelerators
E ~ 0.01 – 350
GeV
The Sun
e
Earth = 6 x 1010 / cm2s
E 0.1 – 17 MeV
The Big Bang, relic
neutrinos
= 330 / cm3
E = 0.0002 eV
Super Nova
SN1987
E 1-80 MeV
Atmospheric ’s
e,,e,1 /cm2s
E0.1– 10000GeV
- -
Spallation
Neutron SourceAli R. Fazely, Miami Conference, December 16 -22, 2015
6
Neutrinos as Cosmic Messengers
Protons: deflected by
magnetic fields. p
Photons: easily
absorbed by CMB
backgrounds.
γ
Neutrinos: not
deflected by magnetic
fields. Low interaction
cross-section.
ν
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Supernova 1987A
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Type II SupernovaOn average, every 30 years or so in our galaxy
a massive star with M > 8M explodes
Gravitational instability due to C, O, and Si fusion
into a Fe – Ni core
Gravity overcomes the electron pressure and collapse
begins; nuclear densities are reached with a core
radius of R ~ 10 km, with E = GM2/R ~ 1059 MeV
Neutrinos are trapped in the neutrino sphere and
materials bounce, cooling of the neutron star by
neutrino emission, shock wave and explosion
Ekin ~ 0.01 E.
99% of the energy is carried off by neutrinos!
Approximately ~ 1058 Neutrinos are Produced!
Ali R. Fazely, Miami Conference, December 16 -22, 2015
SN87A EventsIMB & Kamioka
IMB
KAM
Ali R. Fazely, Miami Conference, December 16 -22, 2015
“I think I can safely say that
nobody understands Quantum
Mechanics” –
- Richard Feynman
The only tool to calculate 𝝂-N cross section
is Quantum Mechanics
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Neutrino Production Sources
ν Energy
10 MeV 80 MeV 350 GeV 20 TeV To GZK (EeV)
Solar & Reactor < 10 MeV
Supernova < 80 MeV
10 MeV < Accelerator < 350 GeV
100 MeV < Atmospheric < 20 TeV
Astrophysical > TeV
Ali R. Fazely, Miami Conference, December 16 -22, 2015
νN Cross Section Calculations
• The calculations also follow these production classifications
for ν Energy.
• The only free nucleon we have is the proton.
• All neutrino interactions with neutrons must occur through a
reaction with a nucleus.
Shell Model, RPA, EFT for Eν < 100 MeV
Impulse Approximation (Fermi Gas Model, Spectral
Functions) for Eν < ~ 1 GeV
Quark Parton Model for Eν > 1 GeV
Ali R. Fazely, Miami Conference, December 16 -22, 2015
νN Cross Section Calculations
Ali R. Fazely, Miami Conference, December 16 -22, 2015
νN Cross Section Calculations
In the cross section equation, the most challenging part to
calculate is the matrix element part.
At low neutrino energies, i.e. reactors, and to some extent
Supernova, |M|2 = |MF|2 + |MGT|2 ⋍ 1 + 3 = 4, from neutron
β-decay.
However, things become more complicated as neutrino
energy increases and nuclear and nucleon structure effects
come into play!
Ali R. Fazely, Miami Conference, December 16 -22, 2015
νN Cross Section Calculations
The nucleon weak current is;
Q-dependence of vector form factors (F1 and F2) can be measured
from e-scattering. The pseudo-scalar is small and the axial form
factor (FA) can only be measured by neutrino scattering from
nucleons.
Ali R. Fazely, Miami Conference, December 16 -22, 2015
νN Cross Section Calculations
Ali R. Fazely, Miami Conference, December 16 -22, 2015
νN Cross Section Calculations
Cross section measurements
Particle data group http://pdg.lbl.govAli R. Fazely, Miami Conference, December 16 -22, 2015
Structure Function Method
Formaggio and Zeller, Rev. Mod. Phys., Vol. 84, No. 3, July–September 2012
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Parameterized Cross SectionsEν < 60 MeV
Vogel & Beacom,Phys. Rev.
D60, 053003 (1999)
Eν < 300 MeV
Strumia and Vissani, Phys.
Lett. B564 42-54, (2003)
Eν > 1.0 PeV, Eν in GeV
R. Gandhi, et al., Astro. Part.
Phys. 52 81, (1996)
Ali R. Fazely, Miami Conference, December 16 -22, 2015
There is an easier way!
Estimate the total neutrino
nucleon cross sections by using
the relation between prime
numbers and their indices.
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Prime Numbers• Prime numbers are numbers that are divisible by themselves
and “one” only. By this definition, 1 is not considered a prime
• It is a formidable mathematical challenge to determine if a number is prime. Many algorithms have been developed to find new prime numbers.
• No method exists linking primes to their positional rank. For example, the 1143rd prime can only be realized by indexing every prime from the first one, 2, to the 1143rd, which is 9221.
• Understanding Primes would lead to appreciating the complexity of composites, twin primes, lonely primes, factorization of semi primes and other number theory problems.
22Ali R. Fazely, Miami Conference, December 16 -22, 2015
PrimesAre there infinitely many primes?The answer is yes!
Euclid (325-265 BC) proved by contradiction that there are indeed infinitely many primes!
Assume that you know the largest prime P. We then form a composite C such that,C = 2 × 3 × 5 × 7 … × P. Then,C + 1 is either a prime or not. If it is a prime then it is larger than P. If it is not a prime, then it cannot be divisible by any of the primes smaller than P. Again the prime has to be larger than P.
23Ali R. Fazely, Miami Conference, December 16 -22, 2015
Prime - Index Relation
24Ali R. Fazely, Miami Conference, December 16 -22, 2015
Prime NumbersIndex Prime
1 2
2 3
3 5
“ “
7 17
8 19
9 23
11 31
“ “
19 67
“ “
114 619
“ “
1143 9221
“ “
1187 961925Ali R. Fazely, Miami Conference, December 16 -22, 2015
Prime-Index Method
The method takes the index of the prime as the energy and the
prime itself then provides the cross section for that energy.
Because there are no units available, we assign the index to be
in units of MeV. Note, the choice of MeV is made because it is
of the order of the neutron-proton mass difference or of the
nuclear binding energy. The cross sections are then expressed in
units of (0.70) of 10-42 cm2 or in units of 0.70 ab (ab stands for
atto - barn = 10-18 barn).
For example, at a neutrino energy of 19 MeV which is the index
of the prime number 67, the cross section is 0.70 × 67 or ~ 47
ab, i.e. 47 × 10-42 cm2.
Ali R. Fazely, Miami Conference, December 16 -22, 2015
νN Cross Sections
27
Energy (MeV σ (p × 0.7)(ab)
2 2.1
. .
5 7.7
“ “
7 11.9
8 13.3
. .
11 21.7
. .
19 47
. .
500 2499.7
. .
1100 5831.7
. .
3500 22826.3Ali R. Fazely, Miami Conference, December 16 -22, 2015
Prime-Index Prediction of 𝝂-N Cross
Sections
Pearson Correlation Coefficients are 0.98 and 0.99 for 𝝂 and 𝝂, respectively
Prime × 0.70
Prime × 0.26
𝝂-N
𝝂-N
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Ultra High Energies
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Astrophysical Muon NeutrinosNorthern Sky The distribution
of reconstructed
muon energy
proxy for events
sample,
compared to the
expected
distributions for
an E-2 flux.
Significance =
3.7σ330 TeV<E<1.4 PeVPRL 115, 081102
(2015)
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Observation of Highest Energy Neutrinos2.6 ± 0.3 PeV, observed June 11, 2014
(ICRC 2015, July 30 to August 6, 2015, The Hague, The Netherlands.)
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Prime-Index Prediction
Prime-Index Prediction
Next Generation, IceCube-Gen2
Ali R. Fazely, Miami Conference, December 16 -22, 2015
A simulated 60-PeV horizontal muon
Ultra High Energies
• Here we use Gauss’s prime number theorem to
generate ν/ν -N cross sections.
• σ (ab) = 0.70 E(MeV)lnE(MeV) (ν-N);
• σ (ab) = 0.26 E(MeV)lnE(MeV) (ν-N)
• Gravity effects and higher dimensions are
proposed that increase ν-N cross sections by
several orders of magnitude.
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Effects of Gravity and Extra DimensionsSolid Black Line is the Prime-Index Relation Prediction!
Tao Han and Dan Hooper, New Journal of Physics 6 (2004) 150
Ali R. Fazely, Miami Conference, December 16 -22, 2015
Conclusions
A simple method is proposed to estimate and predict 𝝂-
N Cross Sections over six decades of neutrino energy
and is compared to experimental data.
The method provides a quick, reliable estimate of
neutrino-nucleon/nucleus cross sections essential to rate
calculations in various neutrino experiments.
The Pearson Correlation Coefficient was calculated to
be 0.98 and 0.99 for neutrinos and antineutrinos,
respectively.
The method predicts rise in cross sections as
suggested by p-brane and extra dimensions.
Question: Why so good?
Ali R. Fazely, Miami Conference, December 16 -22, 2015