Superradiant MeV γ Scattered by a Room-Temperature Spinor Quantum Fluid

Abstract

Recent reports have revealed the rich long-lived Mossbauer phenomenon of 93m Nb, in which it has long been speculated that the delocalized 93m Nb undergoes Bose-Einstein condensation following an increase in the 93m Nb density beyond the threshold of 10 12 cm −3 at room temperature. We now report on the superradiant Rayleigh of the M4 γ at 662 keV scattered into end-fire modes along the long axis of the sample, as evidence of Bose-Einstein condensation. We observed the Arago (Poisson's) spot in order to demonstrate a near-field γ-ray diffraction from a mm-sized γ source, as well as a γ interference beyond the Huygens-Fresnel principle. During the 107-day monitoring period, seven Sisyphus cycles of mode hopping appeared in the superradiance, which demonstrates the optomechanic bistabilty provided by the collective interaction between the spinor quantum fluid and the impinging γs. Condensate-light interaction produces a pm matter-wave grating to become a Fabry-Pérot resonator with a Q-factor on the order of 10 20 , from which end-fired γs lase.

Emergent Supersymmetry in the Visible Kaluza-Klein Fluxes

“…We resolve rigorously the GW signal in Fig. 2 by 𝑙 45 = 10, 𝑚 @ = 5, and 𝑚 9 = 1 using the UV-IR-IR matching in (6), where we have the resonant commensuration of 𝑓 $ 𝑚 @ ⁄ = 𝑓 45 2 ⁄ to synchronize the co-rolling g-wheels between electromagnetism and gravity. The SuSy state shall accordingly return each two GW cycles of 2 𝑓 45 ⁄ , when the MRP ladders complete their rotation by five turns.…”

“…They reveal the homotopy of anapoles by the emergent mass tower, and impose the axial and chiral magnetic currents in the IIB anapole chain, whose couplings yield three plateaux of negative resistance. They reveal the p-orbit of Nb superstrings and resolve the groundbreaking 𝐵 ) ~ 17 mT from 𝑘 J 𝑇 :) , which allows us to fix the numbers in (3), (4),(5), and(6). Three 2𝑁 % ℎ𝑓 * intervals of equal span support the 𝑁 % 𝛼 again, where the factor of 2 arises from the minigap structure of Peierls-paired Mott electrons.…”

“…The peak at 7.5 keV shows the sub-Poissonian photon statistics like a squeezed laser beam, which further reveals its birth identification as one of the gggg. The quarter g from MeV gggg also shows up in an experiment of g scattering [6], which employs an M4 gs at gggg emitted from 𝑁 % nuclei dress on 𝑁 % atoms by means of exciting electrons, phonons, and magnons on 𝑁 % lattice sites. All channels together compose one collective two-level excitation at resonance, which is highly degenerate while conserving ℏ𝜔 3 without any detuning.…”

“…---A. Zee [1] We used dispersed powder magnets to visualize dense fluxes emanating from the 93m Nb Mossbauer gsoliton in an Nb single crystal (see Fig. 1) [2][3][4][5][6][7], which had shown conventional superconductivity a few hours beforehand. It took us almost a decade to realise that the fluxes were nothing but nuclear Dirac strings, which scatter the 662-keV g ray with an extremely large cross section [6].…”

“…1) [2][3][4][5][6][7], which had shown conventional superconductivity a few hours beforehand. It took us almost a decade to realise that the fluxes were nothing but nuclear Dirac strings, which scatter the 662-keV g ray with an extremely large cross section [6]. They are spontaneous Kaluza-Klein (KK) flux compactifications to stabilize moduli like those in [8,9] but in a different context, which are wrapped on the nuclear length scale of 𝑙 !…”