higgsfact.tex:\subsubsection{RFOFO ring coolers}
higgsfact.tex:we employ an RFOFO lattice (regular-FOFO) where the axial field
higgsfact.tex:cells in an RFOFO lattice are identical.
higgsfact.tex:RFOFO lattice was chosen because, unlike in the SFOFO case used in
higgsfact.tex:\caption{Layout of an RFOFO cooling ring. \label{rforing}}
higgsfact.tex:\caption{Three cells of the RFOFO lattice; a) plan, b) side. \label{cells}} 
neufact.tex:\label{RF:fg18.Q}
neufact.tex:shown in Fig.~\ref{RF:fg18.Q}.
newhiggsfact.tex:\subsubsection{RFOFO ring coolers}
newhiggsfact.tex:\subsubsection{RFOFO ring coolers}
newhiggsfact.tex:we employ an RFOFO lattice (regular-FOFO) where the axial field
newhiggsfact.tex:cells in an RFOFO lattice are identical.
newhiggsfact.tex:RFOFO lattice was chosen because, unlike in the SFOFO case used in
newhiggsfact.tex:\caption{Layout of an RFOFO cooling ring. \label{rforing}}
newhiggsfact.tex:\caption{Three cells of the RFOFO lattice; a) plan, b) side. \label{cells}} 
r_and_d.tex:the cooling channel assumes a normal conducting rf (NCRF) cavity gradient of
r_and_d.tex:performance from superconducting rf (SCRF) cavities at this frequency. In
r_and_d.tex:\item  Development and testing of high-gradient normal conducting rf (NCRF)
r_and_d.tex:\item  Development of high-gradient superconducting rf (SCRF) cavities at
r_and_d.tex:high-gradient 201-MHz SCRF cavity. A test area of suitable
r_and_d.tex:carried out, including a high-power 201 MHz NCRF cavity, a large-bore
r_and_d.tex:A prototype 201-MHz SCRF cavity will be completed and tested, initially at
r_and_d.tex:SCRF cavity will include operation in the vicinity of a shielded solenoid