IPAC2013 - List of Authors (Brüning, O.S.)

Paper

Title

Page

Overview of the LHeC Design Study at CERN

40

O.S. Brüning
CERN, Geneva, Switzerland

The LHeC is a potential future lepton-hadron collider project at CERN based on the existing LHC infrastructure. The presentation highlights the main results of the recently published conceptual design report, including the findings of an international review committee that evaluated it. The presentation outlines the planed future studies and R&D activities for the next years.

Slides MOZB201 [11.894 MB]

MOPWO036

Civil Engineering Feasibility Studies for Future Ring Colliders at CERN

969

J.A. Osborne, O.S. Brüning, M. Klein, S. Myers, S. Myers, L. Rossi, C.S. Waaijer, F. Zimmermann
CERN, Geneva, Switzerland
M. Klein
DESY Zeuthen, Zeuthen, Germany

CERN civil engineers are studying the feasibility of future ring colliders to complement the LHC. Infrastructure works typically represent one third of the cost of major physics projects, so it's critical that the construction costs are well understood from the conceptual stage. This poster presents the first results of the feasibility studies for two potential ring colliders at CERN: the racetrack shaped Linac-Ring LHeC and an 80km circular tunnel to house the High Energy LHC (SHE-LHC) and the TLEP. Some of the key civil engineering challenges faced in such large scale projects are presented with particular emphasis on geology, design and risk.

MOPWO054

The LHeC as a Higgs Boson Factory

1017

F. Zimmermann, O.S. Brüning
CERN, Geneva, Switzerland
M. Klein
The University of Liverpool, Liverpool, United Kingdom

The LHeC is designed to collide a new 60 GeV energy electron beam, from a 3-pass ERL, with the 7 TeV energy LHC proton beam. At the present target ep luminosity of 10³³cm^-2s^-1, the LHeC would produce a few 1000 Higgs bosons per year, allowing for precision coupling measurements, especially of the H –> b bbar decay in charged current deep inelastic scattering (ep –> nu H X). With a significant increase of the luminosity, rarer channels become accessible, as the charm decay. Here such an increase, to the level of 10³⁴cm^-2s^-1 or even beyond, is considered from a combination of improvements, namely with a smaller proton beam emittance, with a further reduction of the proton IP beta function, an increase of the proton bunch intensity and with doubling the lepton beam current, compared to the canonical values assumed in the CDR.

MOPWO063

LHeC IR Optics Design Integrated into the HL-LHC Lattice

1034

M. Korostelev, D. Newton, A. Wolski
Cockcroft Institute, Warrington, Cheshire, United Kingdom
O.S. Brüning, R. Tomás
CERN, Geneva, Switzerland
E. Cruz Alaniz, D. Newton, A. Wolski
The University of Liverpool, Liverpool, United Kingdom

The two main drivers for the CDR LHeC IR design were chromaticy and synchrotron radiation. Recently it has been proposed that the LHeC IR proton optics could be integrated into the ATS scheme, which benefits from higher arc beta functions for the correction of chromaticity. In this scenario the distance between the IP and the protron triplet can be increased allowing for a reduction of the IR dipole field and the synchrotron radiation. First feasibility considerations and more in depth studies of the synchrotron radiation effects are presented in this paper.

TUPME055

Strawman Optics Design for the CERN LHeC ERL Test Facility

1694

A. Valloni, O.S. Brüning, R. Calaga, E. Jensen, M. Klein, R. Tomás, F. Zimmermann
CERN, Geneva, Switzerland
S.A. Bogacz, D. Douglas
JLAB, Newport News, Virginia, USA

In preparation for a future Large Hadron electron Collider (LHeC) at CERN, an ERL test facility is foreseen as a test bed for SRF development, cryogenics, and advanced beam instrumentation, as well as for studies of ERL-specific beam dynamics. The CERN ERL test facility would comprise two linacs, each consisting of 4 superconducting 5-cell cavities at 802 MHz, and two return arcs on either side. With an RF voltage of 75 MeV per linac a final electron energy of about 300 MeV is reached. The average beam current should be above 6 mA to explore the parameter range of the future LHeC. In this paper we present a preliminary optics layout.

Paper	Title	Page
MOZB201	Overview of the LHeC Design Study at CERN	40
	O.S. Brüning CERN, Geneva, Switzerland
	The LHeC is a potential future lepton-hadron collider project at CERN based on the existing LHC infrastructure. The presentation highlights the main results of the recently published conceptual design report, including the findings of an international review committee that evaluated it. The presentation outlines the planed future studies and R&D activities for the next years.
	Slides MOZB201 [11.894 MB]

MOPWO036	Civil Engineering Feasibility Studies for Future Ring Colliders at CERN	969
	J.A. Osborne, O.S. Brüning, M. Klein, S. Myers, S. Myers, L. Rossi, C.S. Waaijer, F. Zimmermann CERN, Geneva, Switzerland M. Klein DESY Zeuthen, Zeuthen, Germany
	CERN civil engineers are studying the feasibility of future ring colliders to complement the LHC. Infrastructure works typically represent one third of the cost of major physics projects, so it's critical that the construction costs are well understood from the conceptual stage. This poster presents the first results of the feasibility studies for two potential ring colliders at CERN: the racetrack shaped Linac-Ring LHeC and an 80km circular tunnel to house the High Energy LHC (SHE-LHC) and the TLEP. Some of the key civil engineering challenges faced in such large scale projects are presented with particular emphasis on geology, design and risk.

MOPWO054	The LHeC as a Higgs Boson Factory	1017
	F. Zimmermann, O.S. Brüning CERN, Geneva, Switzerland M. Klein The University of Liverpool, Liverpool, United Kingdom
	The LHeC is designed to collide a new 60 GeV energy electron beam, from a 3-pass ERL, with the 7 TeV energy LHC proton beam. At the present target ep luminosity of 10³³cm^-2s^-1, the LHeC would produce a few 1000 Higgs bosons per year, allowing for precision coupling measurements, especially of the H –> b bbar decay in charged current deep inelastic scattering (ep –> nu H X). With a significant increase of the luminosity, rarer channels become accessible, as the charm decay. Here such an increase, to the level of 10³⁴cm^-2s^-1 or even beyond, is considered from a combination of improvements, namely with a smaller proton beam emittance, with a further reduction of the proton IP beta function, an increase of the proton bunch intensity and with doubling the lepton beam current, compared to the canonical values assumed in the CDR.

MOPWO063	LHeC IR Optics Design Integrated into the HL-LHC Lattice	1034
	M. Korostelev, D. Newton, A. Wolski Cockcroft Institute, Warrington, Cheshire, United Kingdom O.S. Brüning, R. Tomás CERN, Geneva, Switzerland E. Cruz Alaniz, D. Newton, A. Wolski The University of Liverpool, Liverpool, United Kingdom
	The two main drivers for the CDR LHeC IR design were chromaticy and synchrotron radiation. Recently it has been proposed that the LHeC IR proton optics could be integrated into the ATS scheme, which benefits from higher arc beta functions for the correction of chromaticity. In this scenario the distance between the IP and the protron triplet can be increased allowing for a reduction of the IR dipole field and the synchrotron radiation. First feasibility considerations and more in depth studies of the synchrotron radiation effects are presented in this paper.

TUPME055	Strawman Optics Design for the CERN LHeC ERL Test Facility	1694
	A. Valloni, O.S. Brüning, R. Calaga, E. Jensen, M. Klein, R. Tomás, F. Zimmermann CERN, Geneva, Switzerland S.A. Bogacz, D. Douglas JLAB, Newport News, Virginia, USA
	In preparation for a future Large Hadron electron Collider (LHeC) at CERN, an ERL test facility is foreseen as a test bed for SRF development, cryogenics, and advanced beam instrumentation, as well as for studies of ERL-specific beam dynamics. The CERN ERL test facility would comprise two linacs, each consisting of 4 superconducting 5-cell cavities at 802 MHz, and two return arcs on either side. With an RF voltage of 75 MeV per linac a final electron energy of about 300 MeV is reached. The average beam current should be above 6 mA to explore the parameter range of the future LHeC. In this paper we present a preliminary optics layout.