arXiv subjects

K. Ranjan

Publications and source records attributed to K. Ranjan.

4 recordsLinked to original sources

arXiv2012

Study of effects of failure of beamline elements and their compensation in CW superconducting linac

Project-X is the proposed high intensity proton facility to be built at Fermilab, US. First stage of the Project-X consists of superconducting linac which will be operated in continuous wave (CW) mode to accelerate the beam from 2.5 MeV to 3 GeV. The operation at CW mode puts high tolerances on the beam line components, particularly on radiofrequency (RF) cavity. The failure of beam line elements at low energy is very critical as it results in mis-match of the beam with the following sections due to different beam parameters than designed parameter. It makes the beam unstable which causes emittance dilution, and ultimately results in beam losses. In worst case, it could affect the reliability of the machine and may lead to the shutdown of the Linac to replace the failed elements. Thus, it is important to study these effects and their compensation to get smooth beam propagation in linac. This paper describes the results of study performed for the failure of RF cavity & solenoid in SSR0 section.

physics.acc-ph↗

arXiv2012

Calculation of acceptance of high intensity superconducting proton linac for Project X

Project-X is the proposed high intensity proton facility to be built at Fermilab, US. Its Superconducting Linac, to be used at first stage of acceleration, will be operated in continuous wave (CW) mode. The Linac is divided into three sections on the basis of operating frequencies & six sections on the basis of family of RF cavities to be used for the acceleration of beam from 2.5 MeV to 3 GeV. The transition from one section to another can limit the acceptance of the Linac if these are not matched properly. We performed a study to calculate the acceptance of the Linac in both longitudinal and transverse plane. Investigation of most sensitive area which limits longitudinal acceptance and study of influence of failure of beam line elements at critical position, on acceptance are also performed.

physics.acc-ph↗

arXiv2006

Lattice dynamics of MC60 compounds in FCC phase

Phonon dynamics of alkali metal atom, M doped in C60, forming MC60 solids in fcc phase has been studied. The calculations take into account Van-der-Waals and Coulomb interactions for M-C60 and C60-C60 and show fairly good agreement with reported neutron scattering results for RbC60. The calculations have also been done following Rigid Shell Model (RSM). We also perform calculations for specific heat, Gruneisen parameter, thermal expansion and thermal expansion coefficient.

cond-mat.mtrl-sci↗

arXiv2000

Orientational Ordering and Binding in Alkali doped C60 solids

The binding energy of A3C60, a conductor, is described well by an ionic solid type calculation. This succeeds because there is little overlap between molecular wave functions on neighbouring sites, so that electrons are practically localized on-shell. This leads one to believe that even in A4C60 and A6C60 systems such calculation may suffice. However, for large charge on the anion, there is a possibility for some electrons to delocalize and go into the s-band. We calculate binding energy, keeping these delocalised electrons x, as a parameter and minimize the energy w.r.t. it. We take the intermolecular interaction to be arising out of a C-C potential of 6-exp form and a screened Coulomb interaction between the anions and cations and among themselves. Model calculations are presented for K1C60, K3C60, K4C60 and K6C60 for which the minimum energy state shows no delocalisation. Cohesive Energy dependence on Lattice constant is used to calculate Bulk Modulus for all systems. We have got a reasonably good resemblance with experimental values. Further, we observe that the cohesive energy shows poor resemblance with experimental values. Further, delocalisation of a fraction of electron at the centre of double bond show considerable increase in cohesive energy.

cond-mat.mtrl-sci↗