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

NAME

       RNALfold - manual page for RNALfold 2.5.1

SYNOPSIS

       RNALfold [OPTION]...

DESCRIPTION

       RNALfold 2.5.1

       calculate locally stable secondary structures of RNAs

       Compute locally stable RNA secondary structure with a maximal base pair span.  For a sequence of length n
       and  a  base  pair  span  of  L the algorithm uses only O(n+L*L) memory and O(n*L*L) CPU time. Thus it is
       practical to "scan" very large genomes for short RNA structures.  Output consists of a list of  secondary
       structure  components  of  size  <=  L, one entry per line. Each output line contains the predicted local
       structure its energy in kcal/mol and the starting position of the local structure.

       -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:
              Below are command line options which alter the general behavior of this program

       -v, --verbose
              Be verbose

              (default=off)

       -L, --span=INT
              Set the maximum distance between any two pairing nucleotides.

              (default=`150')

              This option specifies the window length L and therefore the upper limit for the  distance  between
              the bases i and j of any pair (i, j), i.e. (j - i + 1) <= L.

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

              (default=off)

       -o, --outfile[=<filename>]
              Print output to file instead of stdout

              This  option  may  be used to write all output to output files rather than printing to stdout. The
              number of output files created for batch input (multiple sequences) depends on  three  conditions:
              (i)  In case an optional filename is given as parameter argument, a single file with the specified
              filename will be written into. If the optional argument is omitted, (ii) FASTA input or an  active
              --auto-id  switch will write to multiple files that follow the naming scheme "prefix.lfold". Here,
              "prefix" is taken from the sequence id as specified in the FASTA header. Lastly, (iii) single-line
              sequence input without FASTA header will be written to a single file  "RNALfold_output.lfold".  In
              case  an  output file already exists, any output of the program will be appended to it.  Since the
              filename argument is optional, it must immediately follow the short option flag to not be mistaken
              as  new  parameter  to  the  program.  For  instance  \'-ornafold.out\'  will  write  to  a   file
              "rnafold.out".   Note:  Any  special  characters  in the filename will be replaced by the filename
              delimiter, hence there is no way to pass an entire directory path through this  option  yet.  (See
              also the "--filename-delim" parameter)

       -i, --infile=<filename>
              Read a file instead of reading from stdin

              The  default  behavior  of RNALfold is to read input from stdin. Using this parameter the user can
              specify an input file name where data is read from.

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

              The default mode of RNALfold 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, RNALfold 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
              Set prefix for automatically generated IDs (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.lfold" where xxxx is the sequence
              number. Note: Setting this parameter implies --auto-id.

       --id-delim=delimiter
              Change prefix delimiter for automatically generated ids.

              (default=`_')

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

              the prefix string and the increasing number for automatically generated IDs

       --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.lfold". With this flag set, no
              truncation of the output filenames is performed, 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).

       --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.

       -z, --zscore[=DOUBLE]
              Limit the output to predictions with a Z-score below a threshold

              (default=`-2')

              This option activates z-score regression using a trained SVM. Any predicted structure that exceeds
              the specified threshold will be ommited from the output.  Since the Z-score threshold is given  as
              a  negative  number, it must immediately preceed the short option to not be mistaken as a separate
              argument, e.g. -z-2.9 sets the threshold to a value of -2.9

       --zscore-pre-filter
              Apply the z-score filtering in the forward recursions

              (default=off)

              The default mode of z-score filtering considers the entire structure space to  decide  whether  or
              not  a  locally  optimal  structure  at  any  position  i  is  reported  or  not.  When using this
              post-filtering step, however, alternative locally optimal structures

              starting at i with higher energy but lower z-score can be easily missed. The

              pre-filter

              option restricts the structure space already in the forward recursions, such

              that

              only optimal solution among those candidates that satisfy the z-score

              threshold are considered. Therefore, good results according to the z-score threshold criterion are
              less likely to be superseded  by  results  with  better  energy  but  worse  z-score.  Note,  that
              activating  this  switch  results  in  higher  computation  time which scales linear in the window
              length.

       --zscore-report-subsumed
              Report subsumed structures if their z-score is less than that of the enclosing structure

              (default=off)

              In default mode, RNALfold only reports locally optimal structures if they are no  constituents  of
              another, larger structure with less free energy. In z-score mode, however, such a larger structure
              may  have a higher z-score, thus may be less informative than the smaller substructure. Using this
              switch activates reporting both, the smaller and the  larger  structure  if  the  z-score  of  the
              smaller is lower than that of the larger.

       -b, --backtrack-global
              Backtrack a global MFE structure.  (default=off)

              Instead  of  just  reporting  the locally stable secondary structure a global MFE structure can be
              constructed that  only  consists  of  locally  optimal  substructures.  This  switch  activates  a
              post-processing  step  that  takes  the  locally  optimal  structures  to  generate the global MFE
              structure which constitutes the MFE value reported in the last line.  The  respective  global  MFE
              structure  is printed just after the inut sequence part on the last line, preceding the global MFE
              score.  Note, that this option implies -o/--outfile since the locally optimal structures  must  be
              read after the regular prediction step! Also note, that using this this option in combination with
              -z/--zscore  implies  --zscore-hard-filter  to  ensure  proper  construction  of  the  global  MFE
              structure!

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

              (default=off)

       --shape=<filename>
              Use SHAPE reactivity data to guide structure predictions.

       --shapeMethod=D/Z/W
              Include SHAPE reactivity data according to a particular method.

              (default=`D')

              The following methods can be used to convert SHAPE reactivities into pseudo energy contributions.

              'D': Convert by using a linear equation according to Deigan et  al  2009.  The  calculated  pseudo
              energies  will  be  applied  for  every  nucleotide  involved  in  a  stacked pair. This method is
              recognized by a capital 'D' in the provided parameter,  i.e.:  --shapeMethod="D"  is  the  default
              setting.  The  slope  'm'  and  the  intercept 'b' can be set to a non-default value if necessary,
              otherwise m=1.8 and b=-0.6. To alter these parameters, e.g. m=1.9  and  b=-0.7,  use  a  parameter
              string  like this: --shapeMethod="Dm1.9b-0.7". You may also provide only one of the two parameters
              like: --shapeMethod="Dm1.9" or --shapeMethod="Db-0.7".

              'Z': Convert SHAPE reactivities to pseudo energies according to Zarringhalam  et  al  2012.  SHAPE
              reactivities  will  be converted to pairing probabilities by using linear mapping. Aberration from
              the observed pairing probabilities will be penalized during the folding recursion.  The  magnitude
              of the penalties can affected by adjusting the factor beta (e.g. --shapeMethod="Zb0.8").

              'W':  Apply  a given vector of perturbation energies to unpaired nucleotides according to Washietl
              et al 2012. Perturbation vectors can be calculated by using RNApvmin.

       --shapeConversion=type
              Convert SHAPE reactivity according to a particular model.

              (default=`O')

              This method allows one to specify the method or  model  used  to  convert  SHAPE  reactivities  to
              pairing (or unpaired) probabilities when using the SHAPE approach of Zarringhalam et al. 2012. The
              following single letter types are recognized:

              'M': Use linear mapping according to Zarringhalam et al. 2012.

              'C': Use a cutoff-approach to divide into paired and unpaired nucleotides (e.g. "C0.25")

              'S':  Skip  the  normalizing  step since the input data already represents probabilities for being
              unpaired rather than raw reactivity values

              'L': Use a linear model to convert the reactivity into a  probability  for  being  unpaired  (e.g.
              "Ls0.68i0.2" to use a slope of 0.68 and an intercept of 0.2)

              'O': Use a linear model to convert the log of the reactivity into a probability for being unpaired
              (e.g. "Os1.6i-2.29" to use a slope of 1.6 and an intercept of -2.29)

   Model Details:
              You may tweak the energy model and pairing rules additionally using the following parameters

       -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)

       -d, --dangles=INT
              Change the dangling end model (default=`2')

              This  option  allows  one  to  change  the  model  "dangling end" energy contributions, i.e. those
              additional contributions from bases adjacent to helices in free ends and multi-loops 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. RNALfold -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.

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

       I.L.  Hofacker,  B.  Priwitzer,  and  P.F.  Stadler  (2004),  "Prediction of Locally Stable RNA Secondary
       Structures for Genome-Wide Surveys", Bioinformatics: 20, pp 186-190

       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

AUTHOR

       Ivo L Hofacker, Peter F Stadler, Ronny Lorenz

REPORTING BUGS

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

SEE ALSO

       RNAplfold(1) RNALalifold(1)

RNALfold 2.5.1                                     April 2024                                        RNALFOLD(1)