A scenario for capture, bunching and rf rotation of µs from a proton source is presented. It consists of a drift section, a variable frequency ~300→180 MHz bunching section, followed by a fixed or variable frequency (~180 MHz) φ-δE rotation section. In 1-D and 3-D simulations (SIMUCOOL and ICOOL), the overall capture performance of the system is similar to that of induction linac + buncher scenarios developed for the neutrino factory.[1] The total rf required for the system is quite modest. Optimization procedures are described.
Common to various front end designs for a muon collider or neutrino factory are costly low frequency...
The possibility of using an induction linac for phase rotation, or equivalently flattening the head ...
Cooling scenarios for a high-luminosity Muon Collider require bunch recombination for optimal lumino...
A scenario for capture, bunching and rf rotation of {mu}'s from a proton source is presented. It con...
A new scenario for capture, bunching and phase-energy rotation of µ’s from a proton source is explor...
Abstract. Scenarios for capture, bunching and phase-energy rotation of µ’s from a proton source have...
We present possible scenarios for capturing the long bunches of a muon source into a string of high-...
The (International Design Report) IDR neutrino factory scenario for capture, bunching, phase-energy ...
We describe a muon capture section to manipulate the longitudinal and transverse phase-space to coll...
A neutrino factory for nu /sub mu / would require a high-power proton beam bombarding a target to pr...
RF and induction linac approaches to phase rotation of the muon bunch have been studied. Shorter acc...
In this note a scheme for the collection, phase rotation and cooling of muons for a neutrino factory...
In a m-storage ring neutrino source, a high-intensity proton source produces pions from a target, an...
Present designs for a muon collider call for a copious source of muons: 5 × 10 14 µ/s distributed ov...
It is widely believed that a neutrino factory would deliver unparallel performance in studying neutr...
Common to various front end designs for a muon collider or neutrino factory are costly low frequency...
The possibility of using an induction linac for phase rotation, or equivalently flattening the head ...
Cooling scenarios for a high-luminosity Muon Collider require bunch recombination for optimal lumino...
A scenario for capture, bunching and rf rotation of {mu}'s from a proton source is presented. It con...
A new scenario for capture, bunching and phase-energy rotation of µ’s from a proton source is explor...
Abstract. Scenarios for capture, bunching and phase-energy rotation of µ’s from a proton source have...
We present possible scenarios for capturing the long bunches of a muon source into a string of high-...
The (International Design Report) IDR neutrino factory scenario for capture, bunching, phase-energy ...
We describe a muon capture section to manipulate the longitudinal and transverse phase-space to coll...
A neutrino factory for nu /sub mu / would require a high-power proton beam bombarding a target to pr...
RF and induction linac approaches to phase rotation of the muon bunch have been studied. Shorter acc...
In this note a scheme for the collection, phase rotation and cooling of muons for a neutrino factory...
In a m-storage ring neutrino source, a high-intensity proton source produces pions from a target, an...
Present designs for a muon collider call for a copious source of muons: 5 × 10 14 µ/s distributed ov...
It is widely believed that a neutrino factory would deliver unparallel performance in studying neutr...
Common to various front end designs for a muon collider or neutrino factory are costly low frequency...
The possibility of using an induction linac for phase rotation, or equivalently flattening the head ...
Cooling scenarios for a high-luminosity Muon Collider require bunch recombination for optimal lumino...