Provided by: vienna-rna_2.5.1+dfsg-1build3_amd64 bug

NAME

       RNAmultifold - manual page for RNAmultifold 2.5.1

SYNOPSIS

       RNAmultifold [OPTION]... [FILE]...

DESCRIPTION

       RNAmultifold 2.5.1

       Compute secondary structures of multiple interacting RNAs

       The  program  works  much  like  RNAfold, but allows one to specify multiple RNA sequences which are then
       allowed to form conncected components. RNA sequences are read from stdin in the usual format,  i.e.  each
       line  of  input corresponds to one sequence, except for lines starting with ">" which contain the name of
       the next sequence(s).  Multiple strands must be concatenated using  the  \'&\'  character  as  separator.
       RNAmultifold  can  compute  MFE,  partition function, corresponding ensemble free energy and base pairing
       probabilities. These properties are either computed  for  a  particular  arrangement  (concatenation)  of
       sequences,  for  the  full  ensemble  of  the complex of input RNAs, or all complexes formed by the input
       sequences up to a specified number of interacting sequences.  Output consists of a PostScript "dot  plot"
       file  containing the pair probabilities, see the RNAfold man page for details.  The program will continue
       to read new sequences until a line consisting of the single character @ or an end of  file  condition  is
       encountered.

       -h, --help
              Print help and exit

       --detailed-help
              Print help, including all details and hidden options, and exit

       --full-help
              Print help, including hidden options, and exit

       -V, --version
              Print version and exit

   General Options:
              Command line options which alter the general behavior of this program

       -v, --verbose
              Be verbose.

              (default=off)

       -j, --jobs[=number]
              Split  batch input into jobs and start processing in parallel using multiple threads. A value of 0
              indicates to use as many parallel threads as computation cores are available.

              (default=`0')

              Default processing of input data is performed in a serial fashion, i.e. one  sequence  pair  at  a
              time.  Using  this switch, a user can instead start the computation for many sequence pairs in the
              input in parallel. RNAmultifold will create as many parallel computation slots  as  specified  and
              assigns  input  sequences  of  the input file(s) to the available slots. Note, that this increases
              memory consumption since input alignments have to be kept in memory until an empty compute slot is
              available and each running job requires its own dynamic programming matrices.

       --unordered
              Do not try to keep output in order with input while parallel processing is in place.

              (default=off)

              When parallel input processing (--jobs flag) is enabled, the order in  which  input  is  processed
              depends  on the host machines job scheduler. Therefore, any output to stdout or files generated by
              this program will most likely not follow the order  of  the  corresponding  input  data  set.  The
              default of RNAmultifold is to use a specialized data structure to still keep the results output in
              order  with  the  input data. However, this comes with a trade-off in terms of memory consumption,
              since all output must be kept in memory for as long as no chunks of  consecutive,  ordered  output
              are  available.  By  setting  this flag, RNAmultifold will not buffer individual results but print
              them as soon as they have been computated.

       --noconv
              Do not automatically substitute nucleotide "T" with "U"

              (default=off)

       --auto-id
              Automatically generate an ID for each sequence.  (default=off)

              The default mode of RNAmultifold is to automatically determine an ID from the input sequence  data
              if  the input file format allows to do that. Sequence IDs are usually given in the FASTA header of
              input sequences. If this flag is active, RNAmultifold ignores any IDs retrieved from the input and
              automatically generates an ID for each sequence. This ID consists of a prefix  and  an  increasing
              number. This flag can also be used to add a FASTA header to the output even if the input has none.

       --id-prefix=prefix
              Prefix for automatically generated IDs (as used in output file names)

              (default=`sequence')

              If  this  parameter  is  set,  each sequence will be prefixed with the provided string. Hence, the
              output files will obey the  following  naming  scheme:  "prefix_xxxx_ss.ps"  (secondary  structure
              plot), "prefix_xxxx_dp.ps" (dot-plot), "prefix_xxxx_dp2.ps" (stack probabilities), etc. where xxxx
              is the sequence number. Note: Setting this parameter implies --auto-id.

       --id-delim=delimiter
              Change the delimiter between prefix and increasing number for automatically generated IDs (as used
              in output file names)

              (default=`_')

              This parameter can be used to change the default delimiter "_" between

              the prefix string and the increasing number for automatically generated ID.

       --id-digits=INT
              Specify the number of digits of the counter in automatically generated alignment IDs.

              (default=`4')

              When  alignments IDs are automatically generated, they receive an increasing number, starting with
              1. This number will always be left-padded by leading zeros,  such  that  the  number  takes  up  a
              certain  width.  Using  this  parameter,  the  width  can be specified to the users need. We allow
              numbers in the range [1:18]. This option implies --auto-id.

       --id-start=LONG
              Specify the first number in automatically generated alignment IDs.

              (default=`1')

              When sequence IDs are automatically generated, they receive an increasing number, usually starting
              with 1. Using this parameter, the first number can be specified to the users  requirements.  Note:
              negative  numbers  are  not  allowed.   Note:  Setting  this  parameter  implies to ignore any IDs
              retrieved from the input data, i.e. it activates the --auto-id flag.

       --filename-delim=delimiter
              Change the delimiting character that is used

              for sanitized filenames

              (default=`ID-delimiter')

              This parameter can be used to change the delimiting character  used  while  sanitizing  filenames,
              i.e.  replacing invalid characters. Note, that the default delimiter ALWAYS is the first character
              of the "ID delimiter" as supplied through the --id-delim option. If the delimiter is a  whitespace
              character  or empty, invalid characters will be simply removed rather than substituted. Currently,
              we regard the following characters as illegal for use in  filenames:  backslash  '\',  slash  '/',
              question  mark  '?', percent sign '%', asterisk '*', colon ':', pipe symbol '|', double quote '"',
              triangular brackets '<' and '>'.

       --filename-full
              Use full FASTA header to create filenames

              (default=off)

              This parameter can be used to deactivate the default behavior of limiting output filenames to  the
              first  word  of  the  sequence  ID.  Consider  the  following  example: An input with FASTA header
              ">NM_0001 Homo Sapiens some gene" usually produces output files with the prefix "NM_0001"  without
              the  additional  data  available in the FASTA header, e.g. "NM_0001_ss.ps" for secondary structure
              plots. With this flag set, no truncation of the output filenames is done,  i.e.  output  filenames
              receive  the  full  FASTA header data as prefixes. Note, however, that invalid characters (such as
              whitespace) will be substituted by a  delimiting  character  or  simply  removed,  (see  also  the
              parameter option --filename-delim).

   Structure Constraints:
              Command line options to interact with the structure constraints feature of this program

       --maxBPspan=INT
              Set the maximum base pair span

              (default=`-1')

       --commands=<filename>
              Read additional commands from file

              Commands  include  hard  and  soft  constraints, but also structure motifs in hairpin and interior
              loops that need to be treeted differently. Furthermore, commands can be set for  unstructured  and
              structured domains.

   Algorithms:
              Select  additional  algorithms  which  should  be  included in the calculations.  The Minimum free
              energy (MFE) and a structure representative are calculated in any case.

       -p, --partfunc[=INT]
              Calculate the partition function and base pairing  probability  matrix  in  addition  to  the  MFE
              structure. Default is calculation of mfe structure only.

              (default=`1')

              In  addition  to  the  MFE structure we print a coarse representation of the pair probabilities in
              form of a pseudo bracket notation, followed by the ensemble free energy.   Note  that  unless  you
              also specify -d2 or -d0, the partition function and mfe calculations will use a slightly different
              energy model. See the discussion of dangling end options below.

              An  additionally  passed  value  to  this  option  changes  the  behavior  of  partition  function
              calculation:

              In order to calculate the partition function but not the pair probabilities

              use the -p0 option and save about

              50% in runtime. This prints the ensemble free energy -kT ln(Z).

       -a, --all_pf[=INT]
              Compute the partition function and free energies not only for the  complex  formed  by  the  input
              sequences  (the  "ABC...  mutimer"), but also of all complexes formed by the input sequences up to
              the number of input sequences, e.g. AAA, AAB, ABB, BBB, etc.

              (default=`1')

              The output will contain the free energies for  each  of  these  species.  Using  -a  automatically
              switches on the -p option.

       -c, --concentrations
              In  addition  to everything listed under the -a option, read in initial monomer concentrations and
              compute the expected equilibrium concentrations of all possible species (A, B, AA, BB, AB, etc).

              (default=off)

              Start concentrations are read from stdin (unless the -f option is used)  in  [mol/l],  equilibrium
              concentrations  are  given  realtive  to  the  sum  of  the inputs. An arbitrary number of initial
              concentrations can be specified (one tuple of concentrations per line).

       -f, --concfile=filename
              Specify a file with initial concentrations for the input sequences.

              The table consits of arbitrary many lines with  multiple  numbers  separated  by  whitespace  (the
              concentration  of the input sequences A, B, C, etc.). This option will automatically toggle the -c
              (and thus -a and -p) options (see above).

       --absolute-concentrations Report absolute instead of relative
              concentrations

              (default=off)

       -S, --pfScale=scaling factor
              In the calculation of the pf use scale*mfe as an estimate for the ensemble free  energy  (used  to
              avoid overflows).

              The  default  is  1.07, useful values are 1.0 to 1.2. Occasionally needed for long sequences.  You
              can also recompile the program to use double precision (see the README file).

       --bppmThreshold=<value>
              Set the threshold for base pair probabilities included in the postscript output

              (default=`1e-5')

              By setting the threshold the base pair probabilities that  are  included  in  the  output  can  be
              varied.  By  default  only those exceeding 1e-5 in probability will be shown as squares in the dot
              plot. Changing the threshold to any other value allows for increase or decrease of data.

       -g, --gquad
              Incoorporate G-Quadruplex formation into the structure prediction algorithm.

              (default=off)

              Note, only intramolecular G-quadruplexes are considered.

   Model Details:
       -T, --temp=DOUBLE
              Rescale energy parameters to a temperature of temp C. Default is 37C.

       -4, --noTetra
              Do not include special tabulated stabilizing energies for tri-, tetra- and hexaloop hairpins.

              (default=off)

              Mostly for testing.

       -d, --dangles=INT
              How to treat "dangling end" energies for bases adjacent to helices in free ends and multi-loops

              (default=`2')

              With -d1 only unpaired bases can participate in at most one dangling end.  With -d2 this check  is
              ignored,  dangling  energies  will be added for the bases adjacent to a helix on both sides in any
              case; this is the default for mfe and partition function folding (-p).   The  option  -d0  ignores
              dangling ends altogether (mostly for debugging).  With -d3 mfe folding will allow coaxial stacking
              of  adjacent  helices  in  multi-loops.  At  the  moment the implementation will not allow coaxial
              stacking of the two interior pairs in a loop of degree 3 and works only for mfe folding.

              Note that with -d1 and -d3 only the MFE computations will be using this  setting  while  partition
              function uses -d2 setting, i.e. dangling ends will be treated differently.

       --noLP Produce structures without lonely pairs (helices of length 1).

              (default=off)

              For partition function folding this only disallows pairs that can only occur isolated. Other pairs
              may still occasionally occur as helices of length 1.

       --noGU Do not allow GU pairs

              (default=off)

       --noClosingGU
              Do not allow GU pairs at the end of helices

              (default=off)

       -P, --paramFile=paramfile
              Read energy parameters from paramfile, instead of using the default parameter set.

              Different  sets  of energy parameters for RNA and DNA should accompany your distribution.  See the
              RNAlib documentation for details on the file format. When passing the placeholder file name "DNA",
              DNA parameters are loaded without the need to actually specify any input file.

       --nsp=STRING
              Allow other pairs in addition to the usual AU,GC,and GU pairs.

              Its argument is a comma separated list of additionally allowed pairs. If the first character is  a
              "-"  then  AB will imply that AB and BA are allowed pairs.  e.g. RNAmultifold -nsp -GA  will allow
              GA and AG pairs. Nonstandard pairs are given 0 stacking energy.

       -e, --energyModel=INT
              Rarely used option to fold sequences from the artificial ABCD... alphabet, where A  pairs  B,  C-D
              etc.  Use the energy parameters for GC (-e 1) or AU (-e 2) pairs.

       --betaScale=DOUBLE
              Set the scaling of the Boltzmann factors (default=`1.')

              The  argument provided with this option enables to scale the thermodynamic temperature used in the
              Boltzmann factors  independently  from  the  temperature  used  to  scale  the  individual  energy
              contributions of the loop types. The Boltzmann factors then become exp(-dG/(kT*betaScale)) where k
              is  the  Boltzmann  constant,  dG  the  free  energy  contribution of the state and T the absolute
              temperature.

REFERENCES

       If you use this program in your work you might want to cite:

       R. Lorenz, S.H. Bernhart, C. Hoener zu Siederdissen, H. Tafer, C. Flamm, P.F. Stadler and  I.L.  Hofacker
       (2011), "ViennaRNA Package 2.0", Algorithms for Molecular Biology: 6:26

       I.L.  Hofacker, W. Fontana, P.F. Stadler, S. Bonhoeffer, M. Tacker, P. Schuster (1994), "Fast Folding and
       Comparison of RNA Secondary Structures", Monatshefte f. Chemie: 125, pp 167-188

       R. Lorenz, I.L. Hofacker, P.F. Stadler (2016), "RNA folding with hard and soft  constraints",  Algorithms
       for Molecular Biology 11:1 pp 1-13

       The energy parameters are taken from:

       D.H.  Mathews,  M.D.  Disney,  D.  Matthew,  J.L. Childs, S.J. Schroeder, J. Susan, M. Zuker, D.H. Turner
       (2004), "Incorporating chemical  modification  constraints  into  a  dynamic  programming  algorithm  for
       prediction of RNA secondary structure", Proc. Natl. Acad. Sci. USA: 101, pp 7287-7292

       D.H  Turner, D.H. Mathews (2009), "NNDB: The nearest neighbor parameter database for predicting stability
       of nucleic acid secondary structure", Nucleic Acids Research: 38, pp 280-282

REPORTING BUGS

       If in doubt our program is right, nature is at fault.  Comments should be sent to rna@tbi.univie.ac.at.

RNAmultifold 2.5.1                                 April 2024                                    RNAMULTIFOLD(1)