Demonstration of Communication Using Neutrinos

Stancil, Daniel D.; Adamson, P.; Alania, M.; Aliaga, L.; Andrews, M.; Castillo, Cesar A.; Bagby, L.; Alba, J. L. Bazo; Bodek, A.; Boehnlein, D.; Bradford, R.; Brooks, W. K.; Budd, H. S.; Butkevich, A.; Caicedo, D. A. Martínez; Capista, D.; Castromonte, C.; Chamorro, Adolfo; Charlton, E.; Christy, M. E.; Chvojka, J.; Conrow, P. D.; Dankó, I.; Day, M.; Devan, J.; Downey, James M.; Dytman, S. A.; Eberly, B.; Fein, Jeffrey; Félix, J.; Fields, L.; Fiorentini, G. A.; Gago, A. M.; Gallagher, H.; Gran, R.; Grange, Joseph; Griffin, Jerry C.; Griffin, T.; Hahn, Eric N.; Harris, Deborah A.; Higuera, A.; Hobbs, John; Hoffman, C. M.; Hughes, B.L.; Hurtado, K.; Judd, A.; Kafka, T.; Kephart, K.; Kilmer, J.; Kordosky, M.; Kulagin, S.; Kuznetsov, V. A.; Lanari, M.; Le, T.; Lee, H.; Loiacono, L.; Mäggi, G.; Maher, E.; Manly, S.; Mann, W. A.; Marshall, C.; McFarland, K. S.; Mislivec, A.; McGowan, A. M.; Morfín, J. G.; Motta, H. da; Mousseau, J.; Nelson, J. K.; Niemiec-Gielata, J. A.; Ochoa, N.; Osmanov, B.; Osta, J.; Palomino, J. L.; Paradis, J. S.; Paolone, V.; Park, J.; Peña, C.; Perdue, G. N.; Lara, Carlos Eugenio Perez; Peterman, A.; Pla‐Dalmau, A.; Pollock, B.; Prokoshin, F.; Ransome, R. D.; Ray, H.; Reyhan, Meral; Rubinov, P.; Ruggiero, Dana; Sands, O. Scott; Schellman, H.; Schmitz, D.; Schulte, E.; Simon, C.; Salinas, C. J. Solano; Stefanski, R. J.; Stevens, Russell; Tagg, N.; Takhistov, Volodymyr; Tice, B. G.; Tilden, R.; Velásquez, J. P.; Vergalosova, I.; Voirin, J.; Walding, J.; Walker, Benjamin; Walton, T.; Wolcott, J.; Wytock, Thomas P.; Zavala, G.; Zhang, D.; Zhu, Liangjia; Ziemer, Benjamin

doi:10.1142/s0217732312500770

Cited by 43 publications

(33 citation statements)

References 11 publications

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“…More importantly, these are not separated fields, rather they are closely interconnected in such a way that advances in one fields sheds light on all other fields as well [1][2][3][4][5][6][7][8][9][10][11][12][13][14].…”

Section: Jhep08(2014)156mentioning

confidence: 99%

Leptonic CP violating effective action for Dirac and Majorana neutrinos

Garcı́a-Recio

Salcedo

2014

J. High Energ. Phys.

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In the Standard Model minimally extended to include massive neutrinos, we compute the leading CP-violating zero temperature contributions to the one-loop effective action induced by integration of the leptons. Such contributions start at operators of dimension six and they are P even for Dirac neutrinos and P even or odd for Majorana neutrinos. Dimension four operators are allowed in the mixed Dirac-Majorana case. It is verified by explicit calculation that CP can be violated in two generation settings for Majorana neutrinos. Using different neutrino scenarios we give upper bounds for the couplings of the CP-violating operators. As a rule, we find that lepton-induced couplings are suppressed as compared to quark-induced couplings, whenever the latter are allowed, nevertheless, through virtual lepton-number violating mechanisms, Majorana neutrinos induce new CP-violating operators not present in the quark or Dirac-neutrino cases.

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Section: Jhep08(2014)156mentioning

confidence: 99%

Leptonic CP violating effective action for Dirac and Majorana neutrinos

Garcı́a-Recio

Salcedo

2014

J. High Energ. Phys.

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“…Recently, communication with a modulated neutrino beam was demonstrated using the NuMI beam line and the MINERvA detector at Fermilab [1]. An important task is the development of alternative schemes of neutrino communication which could be more practical and economical for applications.…”

Section: Introductionmentioning

confidence: 99%

Generation and Detection of a Directed Monoenergetic Neutrino Beam with Hydrogen-Like Ions

Folan¹,

Tsifrinovich²

2017

WJNST

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We consider two possible schemes for generation and detection of a monoenergetic directed beam of neutrinos which may have application to neutrino communication. First, we consider generation of a directed neutrino beam using electron capture beta decay in hydrogen-like ions. Next, we suggest detection of a directed neutrino beam using resonant absorption of a neutrino by a bare nucleus with the generation of a bound electron. This reaction is inverse to electron capture beta decay, and we call it "Bound State Inverse Beta Decay (BSIBD)". We show that the recoil effect can be eliminated by an appropriate choice of velocities for the ions and bare nuclei. Finally, we consider a combination of a solid state source of a directed mono-energetic neutrino beam and its detection using BSIBD.

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“…A paper recently published in Modern Physics Letters A [1] and discussed in several magazines [2][3][4] describes the fi rst successful demonstration of just such a "phone." The phone is the brainchild of an international group of particle physicists, working at Fermi national Accelerator Laboratory in Illinois, and it uses neutrinos (yes, those charge-less, nearly-mass-less elusive particles) for digital messaging.…”

mentioning

confidence: 99%

“…The phone is the brainchild of an international group of particle physicists, working at Fermi national Accelerator Laboratory in Illinois, and it uses neutrinos (yes, those charge-less, nearly-mass-less elusive particles) for digital messaging. In the experiment reported in [1], a series of accelerators at the lab produced an energetic beam of protons, which struck a carbon target, giving rise to pions, kaons, and many other exotic particles. These particles passed through a 675 m helium-fi lled "decay pipe," where most of the particles decayed into neutrinos.…”

mentioning

confidence: 99%