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RNASUBOPT(1) |
User Commands |
RNASUBOPT(1) |
RNAsubopt - manual page for RNAsubopt 2.5.0
RNAsubopt 2.5.0
calculate suboptimal secondary structures of RNAs
Reads RNA sequences from stdin and (in the default -e mode)
calculates all suboptimal secondary structures within a user defined energy
range above the minimum free energy (mfe). It prints the suboptimal
structures in dot-bracket notation followed by the energy in kcal/mol to
stdout. Be careful, the number of structures returned grows exponentially
with both sequence length and energy range.
Alternatively, when used with the -p option, RNAsubopt
produces Boltzmann weighted samples of secondary structures.
- -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
- Command line options which alter the general behavior of this program
- -v, --verbose
- Be verbose. (default=off)
- --noconv
- Do not automatically substitude nucleotide "T" with
"U". (default=off)
- -i, --infile=<filename>
- Read a file instead of reading from stdin.
- The default behavior of RNAsubopt is to read input from stdin. Using this
parameter the user can specify an input file name where data is read
from.
- -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 default filename is
"RNAsubopt_output.sub" if no FASTA header precedes the input
sequences and the --auto-id feature is inactive. Otherwise, output
files with the scheme "prefix.sub" are generated, where the
"prefix" is taken from the sequence id. The user may specify a
single output file name for all data generated from the input by supplying
an optional string as argument to this parameter. In case a file with the
same filename already exists, any output of the program will be appended
to it. 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)
- --auto-id
- Automatically generate an ID for each sequence. (default=off)
- The default mode of RNAsubopt 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, RNAsubopt 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 sequences' FASTA id will be prefixed with
the provided string. FASTA ids then take the form
">prefix_xxxx" where xxxx is the sequence number. Note:
Setting this parameter implies --auto-id.
- --id-delim=STRING
- 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=STRING
- 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.sub". 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).
- Command line options to interact with the structure constraints feature of
this program
- --maxBPspan=INT
- Set the maximum base pair span. (default=`-1')
- -C, --constraint[=<filename>] Apply structural
constraint(s) during
- prediction. (default=`')
- The program first reads the sequence(s), then a dot-bracket like string
containing constraints on the structure. The following symbols are
recognized:
- '.' ... no constraint for this base
- 'x' ... the base is unpaired
- '<' ... the base pairs downstream, i.e. i is paired with j > i
- '>' ... the base pairs upstream, i.e. i is paired with j < i
- '|' ... the corresponding base has to be paired
- '()' ... base i pairs with base j
- Due to historic behavior of this program, all pairing constraints will
only
- disallow pairs that conflict with the constraint. This is usually
sufficient to enforce the constraint, but occasionally a base may stay
unpaired in spite of constraints. Use the --enforceConstraint to
really exclude unpaired states.
- --batch
- Use constraints for multiple sequences. (default=off)
- Usually, constraints provided from input file only apply to a single input
sequence. Therefore, RNAsubopt will stop its computation and quit after
the first input sequence was processed. Using this switch, RNAsubopt
processes multiple input sequences and applies the same provided
constraints to each of them.
- --canonicalBPonly
- Remove non-canonical base pairs from the structure constraint.
(default=off)
- --enforceConstraint
- Enforce base pairs given by round brackets ( ) in structure constraint.
(default=off)
- --shape=<filename>
- Use SHAPE reactivity data in the folding recursions (does not work for
Zuker suboptimals).
- --shapeMethod=STRING
- Specify the method how to convert SHAPE reactivity data to pseudo energy
contributions. (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=STRING
- Specify the method used to convert SHAPE reactivities to pairing
probabilities when using the SHAPE approach of Zarringhalam et al.
(default=`O')
- The following methods can be used to convert SHAPE reactivities into the
probability for a certain nucleotide to be unpaired.
- 'M': Use linear mapping according to Zarringhalam et al.
- '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)
- --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.
- Select the algorithms which should be applied to the given RNA
sequence.
- -e, --deltaEnergy=range
- Compute suboptimal structures with energy in a certain range of the
optimum (kcal/mol).
- Default is calculation of mfe structure only.
- --deltaEnergyPost=range
- Only print structures with energy within range of the mfe after post
reevaluation of energies.
- Useful in conjunction with -logML, -d1 or -d3: while
the -e option specifies the range before energies are re-evaluated,
this option specifies the maximum energy after re-evaluation.
- -s, --sorted
- Sort the suboptimal structures by energy and lexicographical order.
(default=off)
- Structures are first sorted by energy in ascending order. Within groups of
the same energy, structures are then sorted in ascending in
lexicographical order of their dot-bracket notation. See the
--en-only flag to deactivate this second step. Note that sorting is
done in memory, thus it can easily lead to exhaution of RAM! This is
especially true if the number of structures produced becomes large or the
RNA sequence is rather long. In such cases better use an external sort
method, such as UNIX "sort".
- --en-only
- Only sort structures by free energy. (default=off)
- In combination with --sorted, this flag deactivates the second
sorting criteria and sorts structures solely by their free energy instead
of additionally sorting by lexicographic order in each energy band. This
might save some time during the sorting process in situations where
lexicographic order is not required.
- -p, --stochBT=number
- Randomly draw structures according to their probability in the Boltzmann
ensemble.
- Instead of producing all suboptimals in an energy range, produce a random
sample of suboptimal structures, drawn with probabilities equal to their
Boltzmann weights via stochastic backtracking in the partition function.
The -e and -p options are mutually exclusive.
- --stochBT_en=number
- Same as "--stochBT" but also print free energies and
probabilities of the backtraced structures.
- -N, --nonRedundant
- Enable non-redundant sampling strategy. (default=off)
- -S, --pfScale=DOUBLE
- Set scaling factor for Boltzmann factors to prevent under/overflows.
- 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).
- -c, --circ
- Assume a circular (instead of linear) RNA molecule. (default=off)
- -D, --dos
- Compute density of states instead of secondary structures.
(default=off)
- This option enables the evaluation of the number of secondary structures
in certain energy bands around the MFE.
- -z, --zuker
- Compute Zuker suboptimals instead of all suboptimal structures within an
energy band around the MFE. (default=off)
- -g, --gquad
- Incoorporate G-Quadruplex formation. (default=off)
- No support of G-quadruplex prediction for stochastic backtracking and
Zuker-style suboptimals yet).
- -T, --temp=DOUBLE
- Rescale energy parameters to a temperature in degrees centigrade.
(default=`37.0')
- -4, --noTetra
- Do not include special tabulated stabilizing energies for tri-, tetra- and
hexaloop hairpins. (default=off)
- Mostly for testing.
- -d, --dangles=INT
- Specify "dangling end" model 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)
- --logML
- Recompute energies of structures using a logarithmic energy function for
multi-loops before output. (default=off)
- This option does not effect structure generation, only the energies that
are printed out. Since logML lowers energies somewhat, some structures may
be missing.
- -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. RNAsubopt -nsp -GA will allow GA and
AG pairs. Nonstandard pairs are given 0 stacking energy.
- --energyModel=INT
- Set energy model.
- 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.
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
S. Wuchty, W. Fontana, I. L. Hofacker and P. Schuster (1999),
"Complete Suboptimal Folding of RNA and the Stability of Secondary
Structures", Biopolymers: 49, pp 145-165
M. Zuker (1989), "On Finding All Suboptimal Foldings of an
RNA Molecule", Science 244.4900, pp 48-52
Y. Ding, and C.E. Lawrence (2003), "A statistical sampling
algorithm for RNA secondary structure prediction", Nucleic Acids
Research 31.24, pp 7280-7301
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
Ivo L Hofacker, Stefan Wuchty, Walter Fontana, Ronny Lorenz
If in doubt our program is right, nature is at fault. Comments should be sent to
rna@tbi.univie.ac.at.
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