Looking for cosmic neutrino background

1. Introduction

According to the Big Bang theory, neutrinos decoupled from other particles earlier than Cosmic Microwave Background (CMB). Detecting these neutrinos will give direct information of the earliest possible epoch of the Universe we can observe after the Big Bang. This review starts first with a brief summary of Cosmic Neutrino Background (CνB) according to the Big Bang theory with the Standard Model of particle physics except that, as observed, neutrinos are massive rather than massless fundamental particles. There have been ideas on how to detect CνB since 1960s. These proposed detection methods can be classified into two types: direct detection and indirect detection method. The direct detection methods can further be divided into two classes: measurements of energy/momentum transfer from CνB neutrinos to target materials in terms of acceleration of the targets through torsion unbalance or possibly through calorimetry, and measurements of energy of outgoing electrons produced by neutrino capture by β-decaying nuclei. The indirect method basically measures the spectrum of ultra-high energy cosmic rays and identify threshold effects/dips due to interactions between ultra-high energy neutrinos or other cosmic rays from some sources and neutrinos from CνB.

2. The Standard Big Bang Cosmology and its Predictions

According to the standard Big Bang cosmology [1–3] the number density of a relativistic particle of type i of momentum $\overrightarrow{p}$, the energy E_i and the internal degree of freedom g_i (2 for γ, 1 for ν or ν) at temperature T is given by

$\begin{array}{cc}{n}_i=\frac{g_i}{{(2\pi )}^3}{\displaystyle \int f_i}(\overrightarrow{p}){\text{d}}^{\text{3}}p \text{and } {\rho }_i=\frac{g_i}{{(2\pi )}^3}{\displaystyle \int E_i}(\overrightarrow{p})f_i(\overrightarrow{p}){\text{d}}^{\text{3}}p,& (1)\end{array}$

where f_i($\overrightarrow{p}$) = 1/[exp((E_i − μ_i)/T) ± 1)] with chemical potential μ_i (+ for fermion and − for boson). From Equation (1) for a relativistic boson of type i its number density is ζ (3)g_iT³/π² and for a relativistic fermion (3/4)ζ (3)g_iT³/π² where ζ is the Riemann zeta function. Also the energy density is (π²/30)g_iT⁴ for a boson and (7/8)(π²/30)g_iT⁴ for a fermion [3].

The time dependence of the scale factor a(t) of the Universe, when radiation is dominant, is expressed by a(t) ~ t^1/2. By definition the Hubble parameter is the ratio $\dot{a}/a$ and thus H = $\dot{a}/a$ = 1/2t. From the Friedman equation for radiation-dominant epoch, the Hubble parameter is

$\begin{array}{cc}{H}^2=\frac{8\pi G}{3}{\rho }_R=\frac{8\pi G}{3}\frac{{\pi }^2}{30}{g}_{eff}{T}^4=2.76\frac{g_{eff}{T}^4}{M_{Pl}^2},& (2)\end{array}$

where G is the universal gravitational constant, ρ_R is the energy density of radiation, M_Pl is the Planck mass, and g_eff is the total number of effective degrees of freedom of relativistic particles in thermal equilibrium at temperature T which is given by

$\begin{array}{cc}{g}_{eff}={\displaystyle \sum _{i=bosons}{g}_i}+\frac{7}{8}{\displaystyle \sum _{j=fermions}{g}_j}.& (3)\end{array}$

Combining Equations (2, 3), the relation between the time t and the temperature T can be found as

$\begin{array}{cc}t=0.30\frac{M_{Pl}}{\sqrt{g_{eff}}{T}^2}~{\left(\frac{1MeV}{T}\right)}^2\text{ sec}& (4)\end{array}$

When the interaction rate of neutrino Γ_ν becomes smaller than the expansion rate of the Universe i.e., H ~ T²/M_Pl, neutrinos decouple from other particles and stop interacting with them at the decoupling temperature T_ν,dec. Γ_ν is σ_νv_νn_ν where σ_ν ≈ α²T²/m⁴_W is the typical neutrino cross section with the fine structure constant α, W mass m_W, v_ν neutrino velocity ~ c = 1, and the neutrino number density n_ν ∝ T³. Γ_ν is then ~ α²T⁵/m⁴_W. When Γ/H ~ α² M_PlT³/m⁴_W = 1, T corresponds to the neutrino decoupling temperature T_ν,dec ~ (m_W⁴/α² M_Pl)^1/3 ~ 4 MeV [3]. More detailed calculations show that T_ν,dec = 2–3 MeV for ν_e and 3.5 MeV for ν_μ,τ. From Equation (4) the neutrino decoupling occurs at ~0.3–1.0 s after the Big Bang. While CMB provides the information of the Universe at 300,000 years after the Big Bang, the study of nucleosynthesis gives the information of the Universe at ~200–1000 s after the Big Bang [3, 4]. Observation of CνB, therefore, would provide the information of the earliest observable Universe.

2.1. Cosmic Neutrino Background

As described in the previous section neutrinos decouple with electrons, positrons and photons at temperature T~ a few MeV and remain as such until today. Soon after the neutrino decoupling, at about T = 0.5 MeV, e^± pair annihilate into photons and transfer their entropy to these photons. This transfer of entropy to photons effectively slows down the rate of decrease in photon temperature compared with that in neutrino temperature as the Universe expands [3]. Since the entropy of neutrinos is conserved, T_ν = (4/11)^1/3T_γ and, since T^now_γ = 2.7 K, T^now_ν = 1.9 K = 1.7 × 10⁻⁴ eV. Therefore the number density of neutrinos is given by n_ν = (3/22)n_γ = 56 cm⁻³ per flavor. In the standard Big Bang model it is assumed that n_ν = n_ν and neutrinos' chemical potentials are zero. However, in this review it is not assumed, in which case it is convenient to introduce an asymmetry parameter for neutrino with flavor α, ν_α: η_α = (n_να − n_να)/n_γ = [π²/12ζ(3)](ξ_α + ξ³_α/π²)(T_ν/T_γ)³ where ξ_α = μ_α/T with μ_α being the chemical potential of ν_α [5]. A recent study of the primordial He abundance data and WMAP data finds that the sum of the asymmetries of all neutrino flavors, taking into account the effect of neutrino oscillation with the neutrino mixing angle sin²θ₁₃ = 0.04 (0.00), is −0.071 (− 0.064) ≤ η_ν ≤ 0.054 (0.072) (90% C.L.) [6]. At the time of neutrino decoupling (T_ν,dec ~ a few MeV), since we know that neutrino masses are much less than a few MeV, all neutrinos are relativistic (for the status of neutrino masses refer to the review by the Particle Data Group) [7]. However, as the current neutrino temperature is 1.9 K (1.7 × 10⁻⁴ eV), some of neutrinos may be non-relativistic, in which case whether neutrinos are Dirac or Majorana type is important.

From a recent analysis by the Planck collaboration using the CMB and Baryon Acoustic Oscillation (BAO) data, the effective number of relativistic active neutrinos at the time of decoupling of the CMB N_eff is found to be 3.30^+0.51_−0.51, consistent with the existence of three active neutrinos [8]. However, according to the analysis using the Planck, WMAP and BICEP2 data by Giusarma et al., N_eff is found to be 4.00 ± 0.41 [9].

2.2. Clustering of CνB

As we know that neutrino has mass, it is possible that CνB can be trapped in gravitational potential well of some structures in the Universe such as large galaxies and clusters of galaxies when CνB has velocity smaller than the escape velocity. For a large galaxy like Milky Way or a large cluster of galaxies the escape velocities are ~600 or ~2000 km/s, respectively. From the Maxwell–Boltzmann distribution, the average velocity of non-relativistic neutrino of mass m_ν at temperature $T_{\nu },<|{\beta }_{\nu }|>=\sqrt{8k{T}_{\nu }/(\pi m_{\nu })}=\sqrt{4.3\times {10}^{-4}\text{eV}/m_{\nu }}$. Therefore < |v_ν| > = 19,600 (6200) km/s for m_ν = 0.1 (1.0) eV [10]. It seems that only a small fraction of neutrinos can be gravitationally trapped in a large cluster of galaxies. However, detailed simulation that takes into account either the current static mass distribution of the Milky Way (MWnow) or an estimated halo mass distribution before the formation of Milky Way through baryonic compression (NFWhalo) reveals that there may be local neutrino overdensity effect at the position of our solar system [11]. The simulation consists of several types of weakly interacting, self-gravitating particles (cold dark matter and neutrinos) modeled as a multi-component collisionless gas with the Vlasov equation and uses the density profile of cold dark matter (CDM) proposed by Navarro, Frank and White (NFWhalo) [12]. The neutrino overdensity n_ν/ < n_ν >, where < n_ν > is the average neutrino density predicted by the standard Big Bang model, is with the NFWhalo model, 12 and 1.4 for m_ν = 0.6 and 0.15 eV, respectively, and with the MWnow model, 20 and 1.6 for m_ν = 0.6 eV and 0.15 eV, respectively. In the both cases (NFWhalo and MWnow) when m_ν < 0.1 eV, there is no overdensity. Overdensity values 20 and 1.4 correspond to values for the neutrino asymmetry parameter η_ν, 2.7 and 0.19, respectively [11].

3. CνB Detection Methods

Several methods to detect CνB have been proposed and these proposed methods can be divided into three categories: (1) direct detection of coherent CνB elastic scattering with target nuclei through momentum transfer, (2) direct detection by neutrino capture by β-decaying nuclei, and (3) indirect method by finding spectral distortion through CνB interaction with ultra-high energy neutrinos or protons/nuclei from unknown sources.

3.1. Coherent Neutrino Elastic Scattering

In this category, there are two possible methods: use of order G_F effect and of G²_F effect where G_F is the Fermi constant.

3.1.1. Order G_F effect

Coherent elastic scattering occurs when the de Broglie wavelength of CνB h/p_ν ~ h/4T_ν ~ 2.4 mm for relativistic and unclustered neutrinos, or 1.2 mm · 1 eV/m_ν(eV) for clustered non-relativistic neutrinos is much larger than inter-atomic spacing of the target material. When a neutrino with momentum p goes through coherent elastic scattering on the target and emerging with momentum p', a concept of neutrino optics can be introduced with an index of refraction n = p′/p and n − 1 ~ G_F [5]. Uses of neutrino optics were proposed to detect CνB either through refraction [13] or through total reflection [14] as an order G_F effect. However, it was pointed out that the force induced by a linear momentum or energy exchange by neutrinos is canceled out to order G_F when the target is in a uniform neutrino density [15, 16].

The only G_F effect viable for detection of CνB is the method proposed by Stodolsky that uses an energy split of the two spin states of non-relativistic electrons in the target immersed in CνB for which polarized electrons in the target are needed [17]. However, this energy split is proportional to n_ν − n_ν [10, 16]. Following Duda et al. here only their result in an optimistic case of a very large asymmetry favouring ν with n_ν − n_ν ≈ n_ν is presented. Note that for overdensity of 20 (m_ν = 0.6 eV) and of 1.4 (m_ν = 0.15 eV) as estimated by Ringwald et al., n_ν − n_ν = 0.95n_ν and 0.28n_ν, respectively. In this approximation the authors find the energy splits for relativistic (R)/non-relativistic (NR), clustering (C)/non-clustering (NC) and Dirac (D)/Majorana (M) neutrinos: ${(\Delta E)}_R^D={(\Delta E)}_R^M=2\sqrt{2}{g}_A{G}_F|{\beta }_{Earth}|n_{\nu }$, where |β_Earth| = < |β_ν| > is the velocity of the Earth relative to CνB normalized to the speed of light in vacuum c, and g_A is 1/2 for ν_e and −1/2 for ν_{μ, τ}. According to Ringwald et al. < β_ν > = 1.4 × 10⁻³ and 2.2 × 10⁻³ for overdensity of 20 and 1.4, respectively. For non-clustered (NC) non-relativistic neutrinos (NR), ${(\Delta E)}_{NC,NR}^M=2{(\Delta E)}_{NC,NR}^D\simeq 1.7\sqrt{m_{\nu }/(1.7\times {10}^{-4}\xi \text{eV})}{(\Delta E)}_R^D$, and for clustered (C) neutrino non-relativistic (NR) neutrinos ${(\Delta E)}_{C,NR}^D=\sqrt{2}{g}_A{G}_F|{\beta }_{Earth}|n_{\nu }$ and (ΔE)^M_{C, NR} ≃ 0. In the case of Dirac relativistic neutrinos the difference in energy ΔE between the two helicity states of an electron in the direction of CνB induces a torque of magnitude ΔE/π. For a target of mass number A, mass M, and linear dimension R with its moment of inertia I = MR² /γ (γ is a geometric factor), the acceleration due to CνB is a = 10⁻²⁷f(γ/10)(100/A)(1 cm/R)(β_Earth/10⁻³) cm/s² where f is neutrino overdensity n_ν / < n_ν > [10]. The current measurable acceleration using Cavendish type torsion balance mechanism is ~ 10⁻¹³ cm/s² [18]. With possible improvements with the current technology a sensitivity down to 10⁻²³ cm/s² may be achieved [11, 18, 19]. With an optimistic neutrino overdensity of 10, γ = 10, A = 100, and R = 1 cm, the expected acceleration is 10⁻²⁶ cm/s² to be compared with the most optimistic sensitivity to the smallest detectable acceleration of 10⁻²³ cm/s². Even in this optimistic situation, the target mass and size would need to be increased by a factor of 1000.

3.1.2. Order G²_F effect

When the Earth moves through the sea of CνB neutrinos, a target on Earth experiences, by elastic scattering, momentum transfer from neutrinos. In the Earth's rest frame (the laboratory frame) the momentum transfer per scattering is: < Δp >_R ≈ β_Earth(E_ν/c) for relativistic neutrinos, < Δp >_NC,NR = β_Earth(4T_ν/c) = < Δp >_R for non-clustering (NC) non-relativistic (NR) neutrinos, and < Δp >_C,NR ≈ β_Earthcm_ν for clustered (C) non-relativistic (NR) neutrinos. The acceleration by CνB is given by a = Φ_ν(N_Av/A)σ_{ν − A} < Δp > where Φ_ν is the CνB flux, A is the mass number of the target, N_Av is the Avogadro number, and σ_{ν − A} is the neutrino-nucleus cross section. σ_{ν − A} = G²_Fm²_ν/π ≈ 10⁻⁵⁶(m_ν/eV)² cm² for NR neutrinos and = G²_FE²_ν/π ≈ 5 × 10⁻⁶³(T_ν/1.9 K) cm² for R neutrinos. When the target satisfies the aforementioned condition for coherent elastic scattering, the cross section gets a coherent enhancement factor A². Then the acceleration is: a = (N_Av/A)n_ν(G²_F/π)A²F where F = (4T_ν)³β_Earth for R neutrinos, F = m²_ν(4T_ν)β_Earth for NC-NR neutrinos, and F = m³_νv²_ν for C-NR neutrinos [10]. This result includes the nuclear coherent enhancement factor A² but does not include another possible coherent enhancement factor N_c due to the larger de Broglie wavelength of CνB than the target size where N_c = (N_Av/A)ρ (λ_ν)³ with ρ being the density of the target [11, 20, 21]. With this enhancement, Duda et al. found that the acceleration due to CνB a = 2 × 10⁻³⁴f ρ(g cm³) cm/s² for R Dirac/Majorana neutrinos, 3 × 10⁻²⁸f(m_ν(eV))²(T_ν/1.9 K)⁻²ρ(g cm³) cm/s² for NC-NR Dirac neutrinos, and 10⁻²⁷f ρ(g cm³) cm/s² for C-NR Dirac neutrinos. Note that for NR Majorana neutrinos, the corresponding cross sections are reduced by β²_ν ≈ 10⁻⁶. Even with an optimistic scenario of f ρ ~ 100, a ≈ 10⁻²⁵ cm/s² is too small compared with the aforementioned smallest detectable acceleration of 10⁻²³ cm/s².

3.1.3. Experimental status of coherent elastic neutrino nucleus scattering (CENNS)

As described above, the methods proposed in this category relies on the big enhancement factor due to CENNS. Although CENNS has been known since the paper by D. Freedman [22], no observation of this reaction has been made. Recently CENNS attracted close attention and several proposals have been made. Wong et al. and Barbeau et al. propose to use antineutrinos from nuclear reactors [23, 24]. The proposal by Akimov et al. plans to use neutrinos from Stopped-pion Spallation Neutron Source (SSNS) at Oakridge National Laboratory, while Brice et al. propose to utilise neutrinos at the Fermilab Booster Neutrino Beam (BNB) [25, 26].

3.2. Neutrino Capture by CνB-Decaying Nuclei

The first suggestion to use neutrino capture by β-decaying nuclei (NCB) was by Weinberg in 1962 to detect CνB [27]. Electron (anti)neutrino capture by a nucleus N that naturally undergoes beta (positron) decay to the daughter nucleus N′ as ν_e/ν_e + N → N′ + e⁺/e⁻ has no energy threshold on the incident (anti)neutrino energy. In β-decay in which the energy conservation requires M(N) − M(N′) = Q_β > 0 where M(N) and M(N′) are the masses of nucleus of N and N', respectively, and Q_β is the kinetic energy of electron/positron. For massive neutrino of mass m_ν, the electron kinetic energy in NCB is E_e = Q_β + E_ν ≥ Q_β + m_ν, while, neglecting the nucleus recoil energy, E_e ≤ Q_β − m_ν for electrons from β-decay. Thus there is a gap of 2m_ν around Q_β in electron kinetic energy between β-decay and neutrino capture event. Cocco et al. find that the NCB cross section times neutrino velocity can be written as σ_NCBv_ν = 2π²ln2/(At_1/2) where A is a function of E_ν only, when the target nucleus characterized by Q_β and Z is given, and t_1/2 is the half-life of the target nucleus [28]. As β-decay events are the major background source to the NCB, larger ratio of the NCB to β-decay events ~ σ_NCB(v_ν/c)t_1/2 is preferable. Among β-decaying nuclei isotopes ³H and ¹⁸⁷Re have the large ratios 3.0 × 10⁵ and 5.9 × 10⁷, respectively. However, the fact that σ_NCB(v_ν/c) for ³H and ¹⁸⁷Re are 7.8 × 10⁻⁴⁵ cm² and 4.3 × 10⁻⁵² cm², respectively, ³H seems the best choice. Although there is a gap of 2m_ν in the electron kinetic energy between the endpoint of the β-decay and the NCB events, the success of this method depends on the energy resolution whose effect may fill this gap. Cocco et al. estimate the signal (NCB) to the background (β-decay) event ratio R in the outgoing electron kinetic energy region W₀ − Δ < E_e < W₀ where Δ is the energy resolution and W₀ is the endpoint energy. They find that for R = 3 and m_ν = 0.7 (0.3) eV the energy resolution should be better than 0.2 (0.1) eV. The event rate per mole per year is calculated to be 2.85 × 10⁻²[σ_NCB(v_ν/c)/10⁻⁴⁵]cm² yr⁻¹ mol⁻¹. With 100 g of ³H as the target, the event rate per year is, for m_ν = 0.6 eV, 7.5, 90, and 150 events using the standard Fermi-Dirac (FD) distribution, Navarro-Frank-White profile (NFWhalo), and the present day mass distribution of the Milky Way (MWnow), respectively. For m_ν = 0.3 (0.15) eV, the rate is 7.5 (7.5), 23 (10), and 23 (12), respectively, with FD, NFWhalo and MWnow distribution [11].

A calculation by Faessler et al. [29] finds that the NCB rate per year for the ³H target (50 μg) to be used for the KATRIN experiment [30] is 4.2 × 10⁻⁶ n_ν/ < n_ν > which is consistent with the result by Cocco et al. above for the FD distribution with n_ν/ < n_ν > = 1. A similar calculation for 760 g of ¹⁸⁷Re to be used for the MARE calorimetric experiment [31] finds the event rate per year 6.7 × 10⁻⁸ n_ν/ < n_ν >, which is too small for a likely value for n_ν/ < n_ν >.

According to Lazauskas et al. [32], the event rate per year per Mcu (mega-curries = 3.7 × 10¹⁶ decays ~ 2.1 × 10^{25 3}H atoms) for approximately 100 g of ³H is 6.5 × n_ν/ < n_ν > yr⁻¹ Mcu⁻¹, which is also consistent with the result by Cocco et al. As for the required energy resolution to have a reasonable signal to noise ratio of unity, they conclude that the resolution should be a factor of two or more smaller than the neutrino mass m_ν, which is similar to the conclusion by Cocco et al.

Note that the KATRIN experiment's goal for the energy resolution is 0.93 eV and the mass of the ³H source is only 50 μg [30] and to increase the mass of the ³H source or to improve the energy resolution it is necessary to seek a new way to perform this type of experiment. Toward this goal of improvement the Project 8 experiment has started [33]. This experiment utilizes detection of cyclotron radiation from β-decay electron to achieve an improvement in the energy resolution. Another proposal to improve the neutrino mass resolution is to use cold atomic tritium rather than molecular tritium used for the KATRIN experiment to detect both the electron and ³He in the final state of β-decay [34]. Finally the PTOLEMY experiment (Princeton Tritium Observatory for Light-Early Universe Massive-neutrino Yield) is most ambitious [35]. It is based on relic neutrino capture on tritium. It uses, in addition to MAC-E Filter (Magnetic Adiabatic Collimation combined with an Electrostatic Filter) adopted in the KATRIN experiment, a large surface-deposition tritium target, cryogenic calorimeter, RF tracking similar to the Project 8 experiment, and time-of-flight systems to achieve the required background suppression and enough event rate. PTOLEMY plans to use 100-g of atomic tritium as the target which can provide enough event rate.

3.3. Cosmic Rays—CνB Scattering

It is argued that the Universe is opaque to electrons, nucleons and photons at energies higher than 10²³ eV [36]. A more careful consideration finds that the interaction between cosmic ray proton and CMB photon p + γ_CMB → π + N imposes an energy threshold known as Greisen-Zatsepin-Kuzmin (GZK) cutoff E_GZK ≈ 5 × 10¹⁹ eV, beyond which cosmic ray protons do not survive [37, 38]. However, Weiler argues that the only particle that can survive the GKZ cutoff is neutrinos and interactions of ultra-high energy cosmic ray neutrinos with CνB through the Z resonance ν + ν → Z → p + any introduces a dip at certain energy in ultra-high energy neutrino flux. If these neutrinos come from sources with the redshift z = 3.5, this dip occurs at 9 × 10¹⁹ eV. Depending on the three neutrino masses and the value of redshift parameter z of the sources of these ultra-high energy neutrinos, there may be possibly three dips in energy spectrum of cosmic ray neutrinos if these sources exist. The existence of these neutrino sources can produce cosmic rays beyond the GZK cutoff through the Z resonance (Z-burst). However, although the AGASA experiment claimed that they detected cosmic ray events above the GZK cutoff [39], neither the HiRes Experiment [40] nor the Auger experiment [41] confirmed such events.

As for detailed theoretical analyses on the CνB spectroscopy using ultra-high energy cosmic rays, refer to the papers by Barenboim et al. [42] and by D'Olivo et al. [43]. A detailed theoretical analysis on the Z-burst can be found, for example, in the paper by Fargion et al. [44].

Another interaction of cosmic rays with CνB to detect CνB was proposed by Wigman [45]. He proposes to explain, in terms of inverse β-decay interactions such as p + ν_e → n + e⁺, the changes in the power index of cosmic rays spectrum around 10^15.3 eV (the first knee) observed by the CASA-BLANCA experiment [46] from n = 2.72 ± 0.02 to n = 2.95 ± 0.02, and also at the second knee around 10^17.5 eV from n = 3.01 ± 0.06 to n = 3.27 ± 0.02 observed by the Fly's Eye experiment [47]. In the interaction p + ν_e→ n + e⁺ where ν_e is CνB, the center of mass energy $E_{CM}\approx \sqrt{m_p^2+2E_p{m}_{\nu }}$ should be greater than the sum of proton and neutron masses m_p + m_n. This leads to the threshold proton energy for the interaction at 1.695 × 10¹⁵/(m_ν/(1 eV)) eV. If the energy of the knee is, combining several experimental data, at (3 ± 1) × 10¹⁵ eV and the cause of the first knee is the inverse β-decay interaction by proton, it is consistent with the neutrino mass m_νe = 0.5 ± 0.2 eV/c².

Although evidence of high energy cosmic ray neutrinos has finally emerged as the IceCube experiment shows [48], there is only one experimental result that suggests that there are cosmic rays beyond the GZK cutoff, which has not been confirmed by the HiRes and Auger experiment. Various mechanisms in addition to the inverse β-decay theory have been proposed to explain the existence of the knees in cosmic ray spectrum [49]. However, it is not clear which explanation is the correct model for the knees.

4. Future Prospect and Conclusion

In a half-century history of studies on detection of CνB, interesting proposals have been presented. However, with the current available technology, none of the proposed methods that are described in this review are close to be reality, except for the promising Project 8 and PTOLEMY experiment, unless local neutrino overdensity is much larger than expected. For the method to measure the acceleration due to momentum transfer by CνB using torsion balance, the sensitivity of detector needs to be improved by a factor of 1000, even under optimistic circumstances. In addition the contribution from fake signal from various background sources should be carefully evaluated. Detecting CνB by analyzing cosmic ray spectrum as dips beyond the GZK cutoff needs a much larger cosmic ray detector, even if Nature is kind enough to provide ultra-high energy neutrino sources. The existence of the knee-like structures may be explained by other mechanisms than the inverse β-decay. Among β-decaying nuclei as the target, tritium ³H seems to provide the best chance for an NCB experiment to eventually detect CνB if the ideas of the Project 8 and PTOLEMY experiment work to bring better energy resolution and if ~100-g of ³H source, especially, of atomic tritium can be manufactured. However, this method cannot detect ν_μ,τs.

Note added After the submission of this manuscript, a paper by Safdi et al. appeared [50]. This paper describes annual modulation of CνB local density caused by gravitational focusing by the Sun. This modulation can serve as a diagnostic for the signal due to CνB for an experiment based on neutrino capture by β-decaying nuclei.

Conflict of Interest Statement

The author declares that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.

Acknowledgments

This work is in part supported by PSC-CUNY Research Award 66111-00 44.

References

1. Kolb E, Turner M. The Early Universe. Boulder: Westview Press (1994).

2. Weinberg S. Cosmology. New York, NY: Oxford University Press (2007).

3. Bergstroem L, Goobar A. Cosmology and Particle Astrophysics. New York, NY: John Wiley and Sons (1999).

4. Sarkar S. Big bang nucleosynthesis and physics beyond the standard model. Rep Prog Phys. (1996) 59:1493. doi: 10.1088/0034-4885/59/12/001

CrossRef Full Text

5. Gelmini GB. Prospect for relic neutrino searches. In: Proceedings of Nobel Symposium 129 (Enkoping, Sweden) (2005) arXiv:hep-ph/0412305.

6. Castorina E, Franca U, Lattanzi M, Lesgourgues J, Mangano G, Melchiorri A, et al. Cosmological lepton asymmetry with a nonzero mixing angle θ₁₃. Phys Rev. (2012) D86:023517. doi: 10.1103/PhysRevD.86.023517

CrossRef Full Text

7. Beringer J, Arguin JF, Barette RM, Copic K, Dahl O, Groom DE. Review of particle physics. Phys Rev. (2012) D86:010001 (2013 update for the 2014 edition available online at: http://pdg.lbl.gov).

8. Ade PAR, Aghanim N, Armitage-Caplan C, Arnaud M, Ashdown M, Atrio-Barandela F, et al. PLANCK 2013 Results. XVI. Cosmological Parameters. (2013) arXiv:13035076.

9. Giusarma E, Di Valentino E, Lattanzi M, Michiorri A, Mena O. Relic Neutrinos, Thermal Axions and Cosmology in Early 2014. (2014) arXiv:14034852.

10. Duda G, Gelmini G, Nussinov S. Expected signals in relic neutrino detectors. Phys Rev. (2001) D64:122001. doi: 10.1103/PhysRevD.64.122001

CrossRef Full Text

11. Ringwald A, Wong YYY. Gravitational clustering of relic neutrinos and implications for their detection. JCAP. (2004) 0412:005. doi: 10.1088/1475-7516/2004/12/005

CrossRef Full Text

12. Navarro JF, Frank CS, White SDM. The structure of cold dark matter halos. Astrophys J. (1996) 462:563. doi: 10.1086/177173

CrossRef Full Text

13. Opher R. Coherent scattering of cosmic neutrinos. Astron Astrophys. (1974) 37:135.

14. Lewis RR. Coherent detector for low-energy neutrinos. Phys Rev. (1980) D21:663.

15. Cabbibo N, Maiani L. The vanishing of order-G mechanical effects of cosmic massive neutrinos on bulk matter. Phys Lett. (1982) B114:115.

16. Langacker P, Leveille JP, Shaiman J. On the detection of cosmological neutrinos by coherent scattering. Phys Rev. (1983) D27:1228.

17. Stodolsky L. Speculation on detection of the neutrino sea. Phys Rev Lett. (1974) 34:110. doi: 10.1103/PhysRevLett.34.110

CrossRef Full Text

18. Hagmann C. Cosmic neutrinos and their detection. In: Proceedings of DPF 99 Meeting (Los Angeles CA) (1999) arXiv:astro-ph/9905258.

Pubmed Abstract | Pubmed Full Text

19. Hagmann C. A relic neutrino detector. In: Proceedings of the Conference on Particle Physics and the Early Universe. AIP conference proceedings, Vol. 478 (Asilomar, CA) (1998) arXiv:astro-ph/9902102.

Pubmed Abstract | Pubmed Full Text

20. Zel'dovich YB, Khlopov MY. The neutrino mass in elementary-particle physics and in big bang cosmology. Sov Phys Usp. (1981) 24:755. doi: 10.1070/PU1981v024n09ABEH004816

CrossRef Full Text

21. Smith P, Lewin J. Coherent interaction of galactic neutrinos with material targets. Phys Lett. (1983) 127B:185.

22. Freedman D. Coherent effects of a weak neutral current. Phys Rev. (1974) D9:1389.

23. Wong HT, Li HB, Li J, Yue Q, Zhou ZY. Research program towards observation of neutrino-nucleus coherent scattering. J Phys Conf Ser. (2006) 39:266. doi: 10.1088/1742-6596/39/1/064

CrossRef Full Text

24. Barbeau PS, Collar JI, Tench O. Large-mass ultra-low noise germanium detectors: performance and applications in neutrino and astroparticle physics. JCAP. (2007) 09:004. doi: 10.1088/1475-7516/2007/09/009

CrossRef Full Text

25. Akimov D, Bernstein A, Barbeau P, Barton P, Bolozdynya A, Cabrera-Palmer B, et al. Coherent Scattering Investigations at the Spallation Neutron Source: a Snowmass White Paper. (2013) arXiv:13100125.

26. Brice SJ, Cooper RL, DeJongh F, Engel A, Garrison LM, Hime A, et al. A method for measuring coherent elastic neutrino-nucleus scattering at a far off-axis high-energy neutrino beam target. Phys Rev. (2014) D89:072004.

27. Weinberg S. Universal neutrino degeneracy. Phys Rev. (1962) 128:1457. doi: 10.1103/PhysRev.128.1457

CrossRef Full Text

28. Cocco AG, Mangano G, Messina M. Probing low energy neutrino backgrounds with neutrino capture on beta decaying nuclei. JCAP. (2007) 0706:015. doi: 10.1088/1742-6596/110/8/082014

CrossRef Full Text

29. Faessler A, Hodak R, Kovalenko S, Simkovic F. Beta decaying nuclei as a probe of cosmic neutrino background. (2011) arXiv:11021799.

30. Parno DS. The KATRIN experiment: status and outlook. In: Proceedings of the Sixth Meeting on CPT and Lorentz Symmetry (Bloomington, IN) (2013) arXiv:1307.5289.

31. Nucciotti A. The MARE project. J Low Temp Phys. (2008) 151:597. doi: 10.1007/s10909-008-9718-5

CrossRef Full Text

32. Lazauskas R, Vogel P, Volpe C. Charged current cross section for massive cosmological neutrino impinging on radioactive nuclei. J Phys. (2008) G35:025001. doi: 10.1088/0954-3899/35/2/025001

CrossRef Full Text

33. Oblath NS. Project 8: using radio-frequency techniques to measure neutrino mass. In: Proceedings of DPF 2013 (Santa Cruz, CA) (2013) arXiv:1310.0397.

34. Jerkins M, Klein JR, Majors JH, Robicheaux F, Raizen MG. Using cold atoms to measure neutrino mass. New J Phys. (2010) 12:043022. doi: 10.1088/1367-2630/12/4/043022

CrossRef Full Text

35. Betts S, Blanchard WR, Carnevale RH, Chang C, Chens C, Chidzik S. Development of a relic neutrino detection experiment at PTOLEMY. (2013) arXiv:13074738.

36. Weiler T. Resonant absorption of cosmic ray neutrinos by the relic neutrino background. Phys Rev Lett. (1982) 49:234. doi: 10.1103/PhysRevLett.49.234

Pubmed Abstract | Pubmed Full Text | CrossRef Full Text

37. Greisen K. End to the cosmic-ray spectrum? Phys Rev Lett. (1966) 16:748. doi: 10.1103/PhysRevLett.16.748

CrossRef Full Text

38. Zatsepin GT, Kuzmin VA. Upper limit of the spectrum of cosmic rays. JETP Lett. (1966) 4:78.

39. Takeda M, Hayashida N, Honda K, Inoue N, Kadota K, Kakimoto F, et al. Extension of the cosmic-ray energy spectrum beyond the predicted Greisen-Zatsepin-Kuzmin cutoff. Phys Rev Lett. (1998) 81:1163. doi: 10.1103/PhysRevLett.81.1163

CrossRef Full Text

40. Sokolsky P. Final results from the high resolution Fly's Eye (HiRes) experiment. Nucl Phys B. (2013) 212–213:74.

41. Abraham J, Abreu P, Aglietta M, Ahn EJ, Allard D, Allen J, et al. Measurement of the energy spectrum of cosmic rays above 10¹⁸ eV using the Pierre Auger observatory. Phys Lett. (2010) B685:239. doi: 10.1016/j.physletb.2010.02.013

CrossRef Full Text

42. Barenboim G, Requejo OM, Quigg C. Diagnostic potential of cosmic-neutrino absorption spectroscopy. Phys Rev. (2005) D71:083002. doi: 10.1103/PhysRevD.71.083002

CrossRef Full Text

43. D'Olivo JC, Nellen L, Sahu S, Van Elewyck V. UHE neutrino damping in a thermal gas of relic neutrinos. Astropart Phys. (2006) 25:47. doi: 10.1016/j.astropartphys.2005.11.005

CrossRef Full Text

44. Fargion D, Mele B, Salis A. Ultra-high-energy neutrino scattering onto relic light neutrinos in the galactic halo as a possible source of the highest energy extragalactic cosmic rays. Astrophys J. (1999) 517:725. doi: 10.1086/307203

CrossRef Full Text

45. Wigman R. PeV cosmic rays: window on the leptonic era? Astropart Phys. (2003) 19:379. doi: 10.1016/S0927-6505(02)00242-6

CrossRef Full Text

46. Fowler JW, Fortson LF, Jui CCH, Kieda DB, Ong RA, Pryke CL, et al. A measurement of the cosmic ray spectrum and composition at the knee. Astropart Phys. (2001) 15:49. doi: 10.1016/S0927-6505(00)00139-0

Pubmed Abstract | Pubmed Full Text | CrossRef Full Text

47. Watson AA. The highest energy cosmic rays. Nucl Phys B. (1991) 22:116. doi: 10.1016/0920-5632(91)90011-3

CrossRef Full Text

48. Artsen MG, Abbasi R, Abdou Y, Ackermann M, Adams J, Aguilar JA, et al. Evidence for high-energy extraterrestrial neutrinos at the IceCube detector. Science (2013) 342:1242856. doi: 10.1126/science.1242856

Pubmed Abstract | Pubmed Full Text | CrossRef Full Text

49. Bluemer J, Engel R, Hoerandel JR. Cosmic rays from the knee to the highest energies. Prog Part Nucl Phys. (2009) 63:293–338. doi: 10.1016/j.ppnp.2009.05.002

CrossRef Full Text

50. Safdi BR, Lisanti M, Spitz J, Formaggio JA. Annual modulation of cosmic relic neutrinos. (2014) arXiv:14040680.