Input CDCC format

&CDCC namelist

hcm, rmatch, rintp, hnl, rnl, centre, rsp, iter, pset, llmax, dry, rasym, accrcy, switch, ajswtch, sinjmax, cutl, cutr, cutc, absend, jtmin, jump, jbord, nnu, rmatr, nrbases, nrbmin, pralpha, pcon, meigs, listcc, smats, veff, chans, xstabl, thmin, thmax, thinc, smallchan, smallcoup, melfil, nosol, cdetr, numnode, treneg, nlpl, trans, pel, exl, cdccc, qscale, pade, kfus, elab, lab, lin, lex,
hktarg, ncoul, reor, pauli, nk, q, ipc, iscgs, ipcgs, hat, remnant, postprior, quasi, sumform, qc, la, static, expand, maxcoup

are all the same as the &FRESCOX namelist, except for:
cdccc which is an alias for cdcc of &Fresco namelist,
q = ip1, multiple for the projectile single-particle couplings,
ncoul = ip2, selecting nuclear and/or coulomb,
reor = ip3, selecting diagonal and/or off-diagonal couplings,
qc = ip4, $Q_{\rm max}$ for the deformed core potential multipoles,
la = ip5, $\Lambda_{\rm max}$ for the new multipole orders with formfactor reduction,
hat (logical, default T) to use mean bin energies (otherwise midpoint),
quasi: if assigned, set all channel energies as if for this projectile energy (eg -be for adiabatic),
iscgs,ipcgs = isc,ipc (&overlap) for the projectile ground state wave function,
elab = ELAB(1), just the one projectile lab energy,
hktarg = target value of $h.K$, where $h$=HCM and $K$ is the elastic wave number. (default hktarg=0.2).
If HCM=0 in &Fresco namelist, then $h$ is calculated from elab and hktarg.

sumform determines the bin formfactor reductions (default 2 if there are any kind=3 bin states, else 0):
   = 0 : no formfactor reduction: $\langle {\tt KN} \vert K Q \lambda \vert {\tt KNP} \rangle$
= 1 : $KQ\lambda$ formfactors summed into new multipole $\Lambda$: $\langle {\tt KN} \vert \Lambda \vert {\tt KNP} \rangle$
= 2 : formfactors summed into composite projectile state: $\langle {\tt IB} \vert {\Lambda} \vert {\tt IBP} \rangle$. This is not allowed if have spin-orbit or transfer couplings, and sumform=1 will be set in these cases.

If have no cc bins, then $K$ multipoles truncated using ip1=q.
If have cc bins and $Q_{\rm max}$=qc=ip4 and $\Lambda_{\rm max}$=la=ip5 are unset, then q sets the maximum multipole order of $\Lambda$, and all possible values of $KQ\lambda$ are used that couple to $\Lambda \le {\tt q}$
If qc and la are both set, then control each multipole individually:
q = $K_{\rm max}$, ip1 set in usual way
ip4=qc = $Q_{\rm max}$.
ip5=la = $\Lambda_{\rm max}$ maximum order for new multipole.
Note: $\lambda$ will always run from $0\rightarrow Q$.

trans determines the number of transfer partitions:
   = 0 : no transfers: no E(jectile) or R(esidue)
$<$ 0 : only R(esidue): the Ejectile and Core are identical
$>$ 0 : both E(jectile) and R(esidue) independently of Core nucleus.

postprior = ip1 for finite-range transfer couplings,
remnant = ip2 for finite-range transfer couplings,
pauli = attempted Pauli blocking using non-orthogonality couplings.

&NUCLEUS namelist
part,name,mass,charge,spin,parity,be,n,l,j,ia,a,kind,lmax,nch,nce,ampl
where this line is repeated for each part beginning P: projectile, C: core, V: valence, T: target, E: ejectile, R: residue. The number of nuclei (4, 5 or 6) depends on trans: see above.
name,mass,charge as name, mass, zp/t in a &partition namelist,
spin,parity as Jp/t, Bandp/t in a &states namelist.
be,n,l,j,ia,a,kind,lmax,nch prescribe the projectile P bound state, and with transfers also for residue R.
nce is the number of Core excited states.

If nce$>$0, then read that number of &CORESTATES namelists.
&CORESTATES namelist: spin,parity,ex
for spin, parity ($\pm1$) and excitation energy of each Core state above the ground state.

&BIN namelist
spin,parity, step,start,end,energy, n,l,j,isc,ipc, kind,lmax,nch,ia,il,ampl
These are repeated until an empty &BIN namelist is encountered (step=0).
Each bin set has the same spin, parity, l, j, isc, ipc, kind, lmax, nch, ia, il, ampl, but a different energy. The energy range is divided into (end-start)/step bins. If energy then these are evenly spaced in energy, else they are evenly spaced in momentum $k \propto \sqrt{E}$. Changing or starting partial waves is equivalent to start= 0.001.
The values of lmax, nch, ia, il are only needed coupled channels bins kind=3, with il being the channel number of the incoming partial wave, which, if il=0, is defined as the channel with quantum numbers l, j and ia. The array ampl gives overall multiplicative spectroscopic amplitudes to the bin. The values of isc, ipc, kind, lmax have the same meaning as in a &overlap namelist, with j an alias for jn.
If l,j,ia are not set then kind=3 coupled-channels bins are generated using lmax, for all incoming waves. Setting il will select an incoming channel.

&POTENTIAL namelist
part, a1, a2, rc, ac, v, vr0, a, w, wr0, aw, wd, wdr0, awd, vso, rso0, aso, shape, freal, fimag, vsot, rsot0, asot, l, parity, nosub, itt, beta2, beta3, idef, beta2c, beta3c, beta2m, beta3m
where this namelist is repeated for each part beginning P: projectile-target optical potential, C: core-target optical potential, V: valence-target optical potential, T: projectile (C+V) ground state, B: projectile channels not containing the ground state, T: transfer channel optical potential, E: ejectile bound state, R: residue bound state.
Different part=B(in) potentials may be defined depending on parity or partial wave l.
nosub means that the P(rojectile) optical potential is added to the CDCC couplings as a diagonal in all projectile state channels.

For deformations, beta2m, beta3m are the nuclear fractional deformations, and beta2c, beta3c are the Coulomb equivalents (both with default values beta2, beta3 respectively).
The Coulomb and nuclear deformations may also be restricted by idef:
= 0 : Coulomb & nuclear (complex)
= 1 : nuclear (complex) only
= 2 : Coulomb only

Sample CDCC input file:

11Be+4He spdf; 1+5*10+2*5 chs 0-10 MeV, q=0-3 2200 MeV, 30/100 fm
CDCC
 &CDCC
   hcm=0 rmatch=-30 absend=-50 rasym=100 accrcy=0.001
   elab=2200
   jbord=  0   60 200 2500
   jump =  4    5  20
   thmax=30 thinc=.05 smats=2 xstabl=1  cutr=-10 cutc=0
   nk=50 ncoul=0 reor=0 q=3
   /
 &NUCLEUS part='Proj' name='11Be' spin=0.5 parity=+1 be = 0.500 n=2 l=0 j=0.5 /
 &NUCLEUS part='Core' name='10Be' charge=4 mass=10 /
 &NUCLEUS part='Valence' name='neutron' charge=0 mass=1 spin=0.5/
 &NUCLEUS part='Target' name='4He' charge=2 mass=4 /

 &BIN spin=0.5 parity=+1 step=0.5 end=10. energy=F l=0 j=0.5/
 &BIN spin=0.5 parity=-1 step=0.5 end=10. energy=F l=1 j=0.5/
 &BIN spin=1.5 parity=-1 step=0.5 end=10. energy=F l=1 j=1.5/
 &BIN spin=1.5 parity=+1 step=1.0 end=10. energy=F l=2 j=1.5/
 &BIN spin=2.5 parity=+1 step=1.0 end=10. energy=F l=2 j=2.5/
 &BIN spin=2.5 parity=-1 step=2.0 end=10. energy=F l=3 j=2.5/
 &BIN spin=3.5 parity=-1 step=2.0 end=10. energy=F l=3 j=3.5/
 &BIN /

 &POTENTIAL part='Proj' a1=11 a2=4 rc=1.0  /
 &POTENTIAL part='Core' a1=10 a2=4 rc=1.0
            V=46.92 vr0=1.204 a=0.53 W=23.46 wr0=1.328 aw=0.53 /
 &POTENTIAL part='Valence' a1=4 rc=1.3
            V=37.14 vr0=1.17  a=0.75 W=8.12  wr0=1.26  aw=0.58 /
 &POTENTIAL part='Gs' a1=10 v=51.51 vr0=1.39 a=.52 vso=0.38 rso0=1.39 aso=0.52/
 &POTENTIAL part='Bi' a1=10 v=28.38 vr0=1.39 a=.52 vso=0.38 rso0=1.39 aso=0.52/