A scenario for capture, bunching and rf rotation of {mu}'s from a proton source is presented. It consists of a drift section, a variable frequency {approximately} 300 {r_arrow} 180 MHz bunching section, and a fixed (or variable) frequency ({approximately}180 MHz) {phi}-{delta}E 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. The total rf required for the system is quite modest. Optimization procedures are described
Present designs for a muon collider call for a copious source of muons: 5 × 10 14 µ/s distributed ov...
Muon accelerators offer an attractive option for a range of future particle physics experiments. The...
An update is presented on a conceptual design for a pion production target station using a rotating ...
A scenario for capture, bunching and rf rotation of µs from a proton source is presented. It consist...
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...
The possibility of using an induction linac for phase rotation, or equivalently flattening the head ...
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...
The proposed neutrino factory, a facility for precision measurements of neutrino oscillations, requi...
Present designs for a muon collider call for a copious source of muons: 5 × 10 14 µ/s distributed ov...
Muon accelerators offer an attractive option for a range of future particle physics experiments. The...
An update is presented on a conceptual design for a pion production target station using a rotating ...
A scenario for capture, bunching and rf rotation of µs from a proton source is presented. It consist...
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...
The possibility of using an induction linac for phase rotation, or equivalently flattening the head ...
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...
The proposed neutrino factory, a facility for precision measurements of neutrino oscillations, requi...
Present designs for a muon collider call for a copious source of muons: 5 × 10 14 µ/s distributed ov...
Muon accelerators offer an attractive option for a range of future particle physics experiments. The...
An update is presented on a conceptual design for a pion production target station using a rotating ...
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