Sticking probability to the fusion products of a mass-nonsymmetric dtμ molecule

Abstract

An approach is presented for evaluation of the muon ‘sticking probability’ to helium in muon-catalyzed fusion reactions. The probability of initial sticking of muon to helium in the reaction dtμ → μ4He + n is calculated variationally, employing a new wavefunction in a coupled channel method. Our results agree with the previous theoretical report. Moreover, the energy values for such levels below tμ(1s) + d threshold are calculated with a good accuracy and a short computation time.

Use of a posterior pedicle nasal septum and floor mucoperiosteum flap to resurface the nasopharynx after endoscopic nasopharyngectomy for recurrent nasopharyngeal carcinoma

“…We obtain the three coupled integro‐differential equations for variation of the trial wave function. As earlier, we considered the formation of the ordinary ion dtμ produced in the collisions of tμ(1s) + d, using a different set of basis functions 16. At present, we reach to a denser vibrational‐state spectrum of dtμ*, as given in Table I.…”

Resonance energies and fusion rates of mass‐nonsymmetric dtμ* molecule

“…We obtain the three coupled integro-differential equations for variation of the trial wave function. As earlier, we considered the formation of the ordinary ion dt produced in the collisions of t(1s) ϩ d, using a different set of basis functions [16]. At present, we reach to a denser vibrational-state spectrum of dt*, as given in Table I.…”

Elastic cross sections of 1s-muonic atoms at low energies in non-adiabatic approach

“…f ðkÞ JM¼00 l¼00 ð k Þ are the our unknown functions. The definition of Equation (6) is reasonable to reach accurate results in the coalescence points (for comparison see the wave function within [7]). Because we are mainly concerned with low-energy collisions (i.e.…”

“…We employ a trial wave function to calculate s-wave elastic cross-sections using the scattering-theoretic model of Faddeev-Hahn, at the t(1s) þ d scattering. Already, we considered the structure of the dt pseudo nucleus using an alternative method [7]. The wave function of [7] is not applicable for the present problem.…”

“…Already, we considered the structure of the dt pseudo nucleus using an alternative method [7]. The wave function of [7] is not applicable for the present problem. The present approach simplifies the solution procedure and provides correct asymptotic behaviors of the wave function below the three-body break-up threshold.…”