CSIRO Astronomy and Space Science, Australia Telescope National Facility, PO Box 76, Epping, NSW 1710, Australia
The catalogue includes all published rotation-powered pulsars, including those detected only at high energies. It also includes Anomalous X-ray Pulsars (AXPs) and Soft Gamma-ray Repeaters (SGRs) for which coherent pulsations have been detected. However, it excludes accretion-powered pulsars such as Her X-1 and the recently discovered X-ray millisecond pulsars, for example, SAX J1808.4-3658 (Wijnands & van der Klis, Nature, 394, 344, 1998).
The catalogue can be accessed in a number of different ways. The simplest is from a web interface ( http://www.atnf.csiro.au/research/pulsar/psrcat ) allowing listing of the most commonly used pulsar parameters, their uncertainties and reference information. Several options for tabular output format are provided. Currently, a total of 67 predefined parameters are available: see the parameter list in Appendix A of this help file. A facility is provided for plotting of parameter distributions, either as two-dimensional plots or as histograms. Zoom facilities and interactive identication of plotted points are provided. Custom parameters can be defined by combining parameters in expressions using mathematical operators and functions and these can be either listed or plotted. Finally, the sample of pulsars listed or plotted can be limited by logical conditions on parameters, pulsar name (including wild-card names) or distance from a nominated position. These facilities are described in more detail below and links are provided within the web interface to relevant documentation.
After creating a table or plot, accessing the help pages or reference list, use your browser Back funtion to return to the main catalogue page.
For professional astronomers, a more detailed web interface is available allowing access to parameters of specialist interest and use of custom databases which may be either merged with or used in place of the public database. The catalogue can also be accessed using a command-line interface on unix or linux systems. Contact the authors if you would like access to these facilities.
The purpose of this documentation is to provide a description of all the features available. A more basic tutorial is available to guide the user through the web interface (http://www.atnf.csiro.au/research/pulsar/psrcat/Tutorial/intro.html). We encourage you to send us as much feedback (both positive and negative) as possible about the catalogue, interfaces and documentation.
PLEASE NOTE: If you make use of the ATNF Pulsar Catalogue in a
publication, we request that you acknowledge the source of the
information by referencing the paper: Manchester, R. N., Hobbs,
G. B., Teoh, A. & Hobbs, M., Astron. J., 129, 1993-2006 (2005)
(astro-ph/0412641), which gives a full description of the catalogue, and
by quoting the web address
http://www.atnf.csiro.au/research/pulsar/psrcat.
Where practicable, please list the original references for data
used. Reference lists for data in a given table, both in plain text
and in .bbl format, are available from links at the bottom of the table
page.
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Clicking on the pulsar name gives links to other databases which may
contain information about this pulsar. Clicking on a parameter name brings
up the list of parameter descriptions (Appendix A) in which the selected
parameter is highlighted in red.
Custom variables are functions of the predefined variables. Up to
four custom variables (C1, C2, C3 and C4) may be defined. The definition
is provided in the text box. Valid expressions for this definition
are given in section 4 of this documentation.
This custom variable can subsequently be used in sorting,
conditions
or plotted output. If the check-box to the left of the custom variable
label is checked then this variable will be listed in any tabular output
(in exponential form to 6 decimal places). For example, a new variable
(C1) can be defined to equal the square root of the period multiplied by
its derivative -- enter into one of the C1, C2, C3 or C4 text boxes sqrt(p0*p1)
and
click on the check-box to the left of the text:


Often the user will require results from only a selection of pulsars
in the catalogue. Filtering can be carried out on the pulsars' parameters
(described in this section), by the pulsars' names
(section 3.4) or by their position (section
3.5). The conditional expression can be any valid
expression (section 4) with the following conditional
statements:
| == | Equality | != | Inequality test |
| < | Less than | ! | Logical NOT |
| <= | Less than or equal to | && | Logical AND |
| > | Greater than | || | Logical OR |
| >= | Greater than or equal to |
along with the following functions:
exist(pmtot) && exist(pb)
exist(pmra) && error(pmra) < 20
type(radio)
or to select all pulsars which do not emit at radio wavelengths:
!type(radio)
type(radio)
or to select all pulsars which do not emit at radio wavelengths:
!type(radio)
assoc(snr) will select all pulsars with SNR associations.
range(gl,320,50)
will return pulsars within the required range. The coordinate type can be raj, rajd, gl or elong.
It is possible to supply right ascensions in hours, minutes and seconds and declinations in degrees, minutes and seconds as follows:
raj > h19:33 && decj < d-30:00
(note, the use of an 'h' to indicate hours,minutes and seconds and 'd' for degrees). This can also be used within the range function:
range(raj,h23:01,h02:05)
This format requires a colon (i.e. hours/degrees and minutes must be entered; the use of seconds is optional). The functions hms() and dms() may be used to convert to degrees. For example,
raj > hms(19:33) && decj < dms(-30:25)
It is possible to select pulsars that have been individually entered into the "Pulsar names" box. For example:

would produce a table including only the pulsars B0329+54, B1933+16
and J2346-0609. The pulsar names can be separated by a new line,
comma, tab character or spaces. It is advisable to include the `B'
or `J' in front of the pulsar name; if not both the pulsar B1950
and J2000 names will be searched for a match to the entered name.
The name may include the wildcard characters `*' and `?'. For example,
b1933+1? will match PSRs B1933+16, B1933+17 and B1933+15 whereas j004*+*
will match PSRs J0040+5716 and J0048+3412.
The user may wish to obtain all (or a large amount of) the information
stored for a few pulsars. This is possible, but not practical, using
the standard table forms. It is, therefore, possible to type the
names of the pulsars of interest in the `Pulsar names' area and then to
select "Get Ephemeris". Three output formats are available. Short
format provides all the pulsar parameters stored in the catalogue that
are understood by the TEMPO
[external link] pulsar timing package (most of the observed astrometric
and rotational parameters, but no derived parameters). Long
format provides all the information obtainable from the data stored in
the catalogue (all observed, survey and derived parameters) and the Selected
format uses the parameter selections made in the `predefined variables'
section to define which parameters to display. Examples are shown below.
| Short format
JNAME
J1935+1616
|
Long format
JNAME
J1935+1616
|

Equatorial coordinates can be entered using white spaces or colons, for example "19:33:00" is treated in the same manner as "19 33 00", "19 33" and "19:33". It is sometimes necessary to know the angular distance between each pulsar and the central coordinate. Selecting `Show pulsar's distance from centre of this region' will provide a new column in the tabular output giving this angular distance in degrees.
The final table can take five different forms: `short', `short
with errors', `long with last digit errors', `long with errors' or
`publication quality', with 'long with last digit errors' as
default. The short form is used to provide a condensed summary of the
pulsar parameters; periods are given to six decimal places, dispersion
measures to two decimal places etc. It is expected that this
format will be used for producing tables that can be entered directly
into, for instance, plotting packages where the full measured
precision is not required. The short format with errors produces
a similar table, but provides uncertainties on the parameters that
have corresponding errors. The actual value of the parameter is
given to the same number of decimal places as the "short"
format. The uncertainty is given in an exponent format to one
decimal place. The long formats provides the parameters to their
measured precision, their uncertainties and references. From the
web interface it is possible to click on a reference label to obtain
the full bibliographic reference (see section
8). The uncertainty is given as an integer corresponding to the
uncertainty in the last significant figure in the value. For
example, "1.2 2" can be written as "1.2 +/-
0.2". The `publication quality' format gives the parameters to
full precision with corresponding uncertainties given in
parenthesis. For example, 3.4(5) could also have been written as
3.4 +/- 0.5. The bibliographic references are included as a
separate column on the right hand side of the table. The example
below shows the table produced with the different output formats for
the three pulsars with periods less than two milliseconds:
| short: | ![]() |
| short with errors: | ![]() |
| long with last digit errors: | ![]() |
| publication: | ![]() |
Selecting `No header' will produce a table with no header information at the top and with no spaces between groups of five pulsars. If a parameter has been selected, but does not exist in the catalogue (for example, not all pulsars have had their proper motions measured) then the table will contain a `null value'. By default, this null value is set to a '*'. However, the user may enter any string into the Null Value text box to modify this output. For example, the user could enter: "-999.999" or "no value".
Tabular output may be copied to a local disk using the browser 'Save
As' function with Text format. Netscape provides a method of bypassing
the screen display: pressing Shift and the Table button together will copy
the output directly to the local disk. Alternatively, Select, Copy and
Paste functions may be used. Graphical output may be copied to a local
disk using a screen capture program such as xv.
It is possible to display functions of the pulsar parameters as
a graph or as a histogram. For a normal (x-y) graph, the values
to plot are defined as regular expressions (see examples in section
4) and the axes of the graph can be displayed linearly or logarithmically.
The expressions may contain custom-defined variables. In the following
example the user is plotting rotational periods against period derivatives
on a logarithmic scale:


Binary pulsars are indicated in blue, AXP/SGRs are green, high energy pulsars are purple and the remainder in red. It is possible to select a region on the plot using the mouse cursor, clicking and releasing the LH button to define the region. The names of the pulsars lying within these region are displayed to the right of the graph. Clicking on a pulsar name will put cross-hairs on the pulsar's position on the graph. The selected region can be expanded by clicked on `Zoom in' and the graph reverted to its original form by selecting `Reset Plot'.
Histograms can be produced by only entering an expression into the x-axis
text-box. For example to form a histogram of the logarithm of the
rotational periods, type P0 in the x-axis box and select a logarithmic
scale and then click on
.
This will give the following output:

The blue colour represents binary pulsars, green AXP and SGRs and purple high energy pulsars. Clicking on any bar will provide a listing of all the pulsars that lie within that bin of the histogram. The number of bins can be increased or decreased by typing the required number of bins under the Number of bins heading or by clicking on the left and right arrows to decrement or increment the number of bins respectively.
| + | Addition |
| - | Subtraction |
| * | Multiplication |
| / | Division |
| ** | Raise to the power |
| = | assignment |
| acos | inverse cosine | sin | sine of angle in radians |
| asin | inverse sine | sind | sine of angle in degrees |
| atan | inverse tangent | sinh | hyperbolic sine |
| atan2 | inverse tangent | sqr | square |
| cos | cosine of angle in radians | sqrt | square root |
| cosd | cosine of angle in degrees | tan | tan of angle in radians |
| cosh | hyperbolic cosine | tand | tan of angle in degrees |
| exp | exponential | tanh | hyperbolic tangent |
| ln | log (base 2) | fabs | absolute value |
| log | log (base 10) | fmod | modulus (two arguments) |
| log10 | log(base 10) |
Each function (except fmod) takes only one variable or expression which
should be typed immediately after the function name and enclosed in parentheses.
The table below lists the major pulsar surveys. The category 'misc'
lists pulsars discovered in other (more limited) searches.
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Reference Keys |
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| ar1 | Arecibo Survey 1 | ht75 | 4 | 49 | 41 |
| ar2 | Arecibo Survey 2 | sstd86 | 400 | 24 | 6 |
| ar3 | Arecibo Survey 3 | nft95 | 2000 | 61 | 24 |
| ar4 | Arecibo Survey 4 | wol90a,cnt93,fwc93,nft93,tdk+93,cam95a,
fcwa95,cnt96,cnst96,rtj+96,snt97,lwf+04, lxf+05 |
20000 | 120 | 74 |
| palfa | Arecibo Multibeam Survey | cfl+06,lsf+06,hng+08,dcm+09,kac+10,kla+11,dfc+12,csl+12 | 2000000 | 55 | 26 |
| FermiBlind | Fermi Gamma-ray Observatory blind survey | aaa+09c,sdz+10,rkp+11,awd+12,pga+12,pga+12a | 4000000 | 37 | 37 |
| FermiAssoc | Searches of unidentified Fermi gamma-ray sources | rrc+11,kjr+11,ckr+12,gfc+12,kcj+12,rap+12,bgc+13 | 20000000 | 39 | 39 |
| gb1 | Green Bank Northern Hemisphere survey | dth78 | 20 | 50 | 31 |
| gb2 | Princeton-NRAO survey | dtws85 | 40 | 83 | 34 |
| gb3 | Green Bank short-period survey | stwd85 | 200 | 86 | 20 |
| gb4 | Green Bank fast pulsar survey | nst96,snt97 | 10000 | 83 | 5 |
| gb350 | Green Bank 350 MHz drift-scan survey | hrk+08,rsm+12,blr+13,lbr+13 | 40000000 | 59 | 58 |
| htru | Parkes high time resolution survey | kjv+10,lbb+10,bbb+11a,kjb+12,bbb+12 | 10000000 | 813 | 86 |
| jb1 | Jodrell A survey | dls77 | 2 | 51 | 37 |
| jb2 | Jodrell B survey | cl86 | 100 | 62 | 42 |
| mol1 | 1st Molonglo survey | vl70 | 1 | 34 | 31 |
| mol2 | 2nd Molonglo Survey | mlt+78 | 10 | 224 | 155 |
| pks1 | Parkes 20-cm survey | jlm+92 | 1000 | 100 | 46 |
| pks70 | Parkes Southern Sky survey | mld+96,lml+98 | 4000 | 298 | 101 |
| pkshl | Parkes high-latitude multibeam pulsar survey | bdp+03,lbk+04,bjd+06 | 1000000 | 42 | 18 |
| pksgc | Parkes globular cluster survey | mld+90,mlr+91,rlm+95,clf+00,dlm+01,dfp+02,pdm+03,fre08 | 200000 | - | 33 |
| pksmb | Parkes multibeam pulsar survey | mlc+01,mhl+02,kbm+03,hfs+04,fsk+04,lfl+06,kle+09,kel+09,mlb+12,kek+13,elkl13 | 40000 | 1114 | 825 |
| pkssw | Parkes-Swinburne multibeam survey | ebvb01,jbv+03,jac04a,jbo+09,bb10 | 100000 | 243 | 108 |
| pkspa | Parkes Perseus Arm multibeam survey | bkl+13 | 100000000 | 15 | 15 |
| misc | -- | 400000 | - | 306 |
The Galactocentric coordinate system (XX, YY, ZZ) is right-handed
with the Sun at (0.0, 8.5 kpc, 0.0) and the ZZ axis directed toward
the north Galactic pole.

the `Name' and `Email' boxes are not compulsory, but should be included
if you require a reply to your comment.
The catalogue database will be upgraded both in response to user
feedback and to include data from recent publications.
Type the name of your database file in the box, using the Browse
function to find the correct directory if necessary. Then hit the
"Upload to ATNF" button and the file will be transferred to an ATNF
disk. A message will report whether or not the upload was successful.
This operation may be repeated to transfer multiple files.
To merge the file(s) with the public database, with precedence given
to later files in the list, click on the Merge button.
Then you may create a table or plot as usual by selecting parameters and
clicking the appropriate button.
If you click the "Delete file immediately after use" button, the
file(s) will be deleted from the ATNF disk after the next operation
(table or plot). Otherwise, they will be left there
indefinitely. However, we
reserve the right to delete files more than one year old.
The current catalogue database and the PSRCAT source code may
be downloaded by clicking on the "Download" link at the top of the
Catalogue webpage.
PSRCAT is free software: you can redistribute it and/or modify
it under the terms of the GNU General Public License as published by
the Free Software Foundation, either version 3 of the License, or
(at your option) any later version.
PSRCAT is distributed in the hope that it will be useful,
but WITHOUT ANY WARRANTY; without even the implied warranty of
MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
GNU General Public License for more details.
PSRCAT makes use of "evaluateExpression: A Simple Expression Evaluator".
Copyright (c) 1996 - 1999 Parsifal Software, All Rights Reserved.
9.1 Custom databases
We regret that, because of hacking problems, the upload facility has been disabled.
In 'Expert' mode, the user is able to upload to the ATNF system one or
more custom databases to be displayed by the web interface. This
facility is also available in the command-line interface version of
psrcat. These databases may either replace the public database or be
merged with it.
9.1.1 Uploading a custom database
At the bottom of the page, there is a section called "Attach your own
Catalogue" as shown below:

9.1.2 Using a custom database
Type the name of your file in the box immediately above, labelled
"File Name:" as shown in the example below. Multiple file names may be
entered, separated by commas or spaces.

10. Downloading the Catalogue
Acknowledgements
The web interface was designed and constructed by Albert
Teoh, during his tenure as a Summer Vacation Scholar at the ATNF,
2002/2003.
This work has made extensive use of NASA's
Astrophysics Data System and the
Google search engine.
The original database was compiled with the invaluable assistance of
Maryam Hobbs during her term as a Research Assistant in the ATNF
Parkes Pulsar Timing Array (PPTA) group (10/2003 - 4/2005). Since then
this work has been continued by Diana Londish (8/2005 - 10/2006),
Lucyna Kedziora-Chudczer (11/2006 - 6/2009), Ankur Chaudhary (9/2009 -
9/2012) and Lawrence Toomey (12/2012 - present).
We thank W. Becker for a pre-publication copy of "X-ray Emission from
Pulsars and Neutron Stars", in "Neutron Stars and Pulsars",
Astrophys. Space Sci. Library 357 (2008), Thomas Tauris and
Paulo Freire for assistance with compiling the list of binary
companion types and relevant references (see Tauris, Langer and
Kramer, 2012, MNRAS, 425, 1601) and Meng Yu for updates to the glitch
table. We acknowledge the use of Paulo Freire's website
Pulsars in Globular Clusters and the
McGill AXP/SGR Online Catalog
which have provided valuable cross-checks and, in some cases, otherwise
unpublished data. Finally, we thank our colleagues for their many
comments and suggestions which have helped to improve both the
database and the means of accessing it.
Appendix A: The Pulsar
Parameters
Name: Pulsar name. The B name if exists, otherwise the J name.
JName: Pulsar name based on J2000 coordinates
RAJ: Right ascension (J2000) (hh:mm:ss.s)
DecJ: Declination (J2000) (+dd:mm:ss)
PMRA: Proper motion in the right ascension direction (mas/yr)
PMDec: Proper motion in declination (mas/yr)
PX: Annual parallax (mas)
PosEpoch: Epoch at which the position is measured (MJD)
ELong: Ecliptic longitude (degrees)
ELat: Ecliptic latitude (degrees)
PMElong: Proper motion in the ecliptic longitude direction (mas/yr)
PMElat: Proper motion in ecliptic latitude (mas/yr)
GL: Galactic longitude (degrees)
GB: Galactic latitude (degrees)
RAJD: Right ascension (J2000) (degrees)
DecJD: Declination (J2000) (degrees)
Bname: Pulsar Besselian name
PML: Proper motion in Galactic longitude (mas/yr)
PMB: Proper motion in Galactic latitude (mas/yr)
Timing solution and profile parameters:
P0: Barycentric period of the pulsar (s)
P1: Time derivative of barcycentric period (dimensionless)
F0: Barycentric rotation frequency (Hz)
F1: Time derivative of barycentric rotation frequency (s-2)
F2: Second time derivative of barycentric rotation frequency (s-3)
F3: Third time derivative of barycentric rotation frequency (s-4)
PEpoch: Epoch of period or frequency (MJD)
DM: Dispersion measure (cm-3 pc)
DM1: First time derivative of dispersion measure (cm-3 pc yr-1)
RM: Rotation measure (rad m-2)
W50: Width of pulse at 50% of peak (ms). Note, pulse widths are a function of both observing frequency and
observational time resolution,so quoted widths are indicative only. Refer to the original reference for details.
W10: Width of pulse at 10% (ms). Note the comments above for W50.
Tau_sc: Temporal broadening of pulses at 1 GHz due to interestellar scattering (s)
S400: Mean flux density at 400 MHz (mJy)
S1400: Mean flux density at 1400 MHz (mJy)
S2000: Mean flux density at 2000 MHz (mJy)
F4: Fourth time derivative of barycentric rotation frequency (s^-5)
F5: Fifth time derivative of barycentric rotation frequency (s^-6)
F6: Sixth time derivative of barycentric rotation frequency (s^-7)
F7: Seventh time derivative of barycentric rotation frequency (s^-8)
F8: Eighth time derivative of barycentric rotation frequency (s^-9)
F9: Ninth time derivative of barycentric rotation frequency (s^-10)
FA: Tenth time derivative of barycentric rotation frequency (s^-11)
FB: Eleventh time derivative of barycentric rotation frequency (s^-12)
FC: Twelfth time derivative of barycentric rotation frequency (s^-13)
DM2: Second time derivative of dispersion measure (cm-3pc yr-2)
DM3: Third time derivative of dispersion measure (cm-3pc yr-3)
DM4: Fourth time derivative of dispersion measure (cm-3pc yr-4)
DM5: Fifth time derivative of dispersion measure (cm-3pc yr-5)
DM6: Sixth time derivative of dispersion measure (cm-3pc yr-6)
DM7: Seventh time derivative of dispersion measure (cm-3pc yr-7)
DM8: Eighth time derivative of dispersion measure (cm-3pc yr-8)
DM9: Ninth time derivative of dispersion measure (cm-3pc yr-9)
S600: Flux at 600 MHz (mJy)
S700: Flux at 700 MHz (mJy)
S800: Flux at 800 MHz (mJy)
S900: Flux at 900 MHz (mJy)
S1600: Flux at 1600 MHz (mJy)
S3000: Flux at 3000 MHz (mJy)
SPINDX: Radio spectral index
Binary system parameters:
Binary: Binary model (usually one of several recognised by the pulsar timing programs TEMPO or TEMPO2
T0: Epoch of periastron (MJD)
PB: Binary period of pulsar (days)
A1: Projected semi-major axis of orbit (lt s)
OM: Longitude of periastron (degrees)
ECC: Eccentricity
TASC: Epoch of ascending node(MJD) - ELL1 binary model
Eps1: Ecc x sin(OM) - ELL1 binary model
Eps2: Ecc x cos(OM) - ELL1 binary model
MinMass: Minimum companion mass assuming i=90 degrees and neutron star mass is 1.35 Mo
MedMass: Median companion mass assuming i=60 degrees
BinComp: Companion type
OMDOT: Periastron advance (deg/yr)
PBDOT: 1st time derivative of binary period
A1DOT: Rate of change of projected semi-major axis
ECCDOT: Rate of change of eccentricity
GAMMA: Post-Keplerian gamma term (s)
T0_2: Epoch of periastron [2nd orbit] (MJD)
PB_2: Binary period of pulsar [2nd orbit] (days)
A1_2: Projected semi-major axis of orbit [2nd orbit] (s)
OM_2: Longitude of periastron [2nd orbit] (deg)
OMDOT_2: Periastron advance [2nd orbit] (deg/yr)
ECC_2: Eccentricity [2nd orbit]
PBDOT_2: 1st time derivative of binary period [2nd orbit]
T0_3: Epoch of periastron [3rd orbit] (MJD)
PB_3: Binary period of pulsar [3rd orbit] (days)
A1_3: Projected semi-major axis of orbit [3rd orbit] (s)
OM_3: Longitude of periastron [3rd orbit] (deg)
OMDOT_3: Periastron advance [3rd orbit] (deg/yr)
ECC_3: Eccentricity [3rd orbit]
PBDOT_3: 1st time derivative of binary period [3rd orbit]
PPNGAMMA: PPN parameter gamma (s)
SINI: Sine of inclination angle
SINI_2: Sine of inclination angle [2nd orbit]
SINI_3: Sine of inclination angle [3rd orbit]
MTOT: Total system mass (solar masses)
M2: Companion mass (solar masses)
M2_2: Companion mass [2nd orbit] (solar masses)
M2_3: Companion mass [3rd orbit] (solar masses)
DTHETA: Relativistic deformation of the orbit
XOMDOT: Rate of periastron advance minus GR prediction (deg/yr)
XPBDOT: Rate of change of orbital period minus GR prediction
DR: Relativistic deformation of the orbit (not fitted)
A0: Aberration parameter A0 (s, not fitted)
B0: Aberration parameter B0 (s, not fitted)
BP: Tensor multi-scalar parameter beta-prime (not fitted)
BPP: Tensor multi-scalar parameter beta-prime-prime (not fitted)
MASSFN: The pulsar mass function (solar mass)
UPRMASS: 90% confidence upper companion mass limit, i=26deg (solar mass)
MINOMDOT: Minimum omega dot, assuming sin i = 1 and M_ns = 1.4Mo (deg/yr)
Distance parameters:
Dist: Best estimate of the pulsar distance using the tc93 DM-based distance as default (kpc)
Dist_DM: Distance based on the tc93 electron density model.
In `LONG' or `PUBLICATION QUALITY' modes, lower limits from the distance model are preceded by a `+' sign.
DMsinb: DM x sin(b) (cm-3 pc)
ZZ: Distance from the Galactic plane, based on Dist
XX: X-Distance in X-Y-Z Galactic coordinate system (kpc)
YY: Y-Distance in X-Y-Z Galactic coordinate system (kpc)
Dist_DM1: Distance based on NE2001 model (kpc)
Dist1: Best estimate of the pulsar distance using the NE2001 DM-based distance as default (kpc)
Dist_A: Independent distance estimate - takes precedence over other distance estimates for DIST and DIST1 (kpc)
Dist_AMN: Lower limit on independent distance estimate (kpc)
Dist_AMX: Upper limit on independent distance estimate (kpc)
Associations and survey parameters:
Assoc: Names of other objects, e.g., supernova remnant, globular cluster or gamma-ray source
associated with the pulsar
Survey: Surveys that detected the pulsar (discovery survey first). Click here for currently defined surveys.
OSurvey: Surveys that detected the pulsar encoded as bits in integer
Date: Date of discovery publication.
Type: Type codes for the pulsar. Click here for available types.
NGlt: Number of glitches observed for the pulsar
TRES: RMS timing residual (microsec)
NTOA: Number of TOAs in timing fit
START: Epoch of start of fit (MJD)
FINISH: Epoch of end of fit (MJD)
CLK: Terrestrial time standard
EPHEM: Solar system ephemeris
TZRMJD: Reference TOA (MJD)
TZRFRQ: Frequency of reference TOA (MHz)
TZRSITE: One-letter observatory code for reference TOA
TDMP: Ideal subintegration time for pulsar (s)
TDMPMIN: Minimum subintegration time for pulsar (s)
NSPAN: Minutes for polyco span
NCOEF: Number of coefficients in polyco
NBIN: Number of bins in the profile
NSUB: Number of subbands to store
GLEP: Epoch of glitch
GLPH: Phase increment at glitch
GLF0: Permanent pulse frequency increment at glitch
GLFI: Permanent frequency derivative increment at glitch
GLF0D: Decaying frequency increment at glitch
GLTD: Time constant for decaying frequency increment
Derived parameters:
R_Lum: Radio luminosity at 400 MHz (mJy kpc2)
R_Lum14: Radio luminosity at 1400 MHz (mJy kpc2)
Age: Spin down age (yr) [
]
BSurf: Surface magnetic flux density (Gauss) [
]
Edot: Spin down energy loss rate (ergs/s)
Edotd2: Energy flux at the Sun (ergs/kpc2/s)
PMTot: Total proper motion (mas/yr)
VTrans: Transverse velocity - based on DIST (km/s)
P1_i: Period derivative corrected for proper motion effect
Age_i: Spin down age from P1_i (yr)
BSurf_i: Surface magnetic dipole from P1_i (gauss)
Edot_i: Spin down energy loss rate from P1_i (ergs/s)
B_LC: Magnetic field at light cylinderUser Parameters
PAR1: A non-standard parameter entered by the user
PAR2: A non-standard parameter entered by the user
PAR3: A non-standard parameter entered by the user
PAR4: A non-standard parameter entered by the user
AXP Anomalous X-ray Pulsar or Soft Gamma-ray Repeater with detected pulsations BINARY Pulsar has one or more binary companions HE Spin-powered pulsar with pulsed emission from radio to infrared or higher frequencies NRAD Spin-powered pulsar with pulsed emission only at infrared or higher frequencies RADIO Pulsars with pulsed emission in the radio band RRAT Pulsars with intermittently pulsed radio emission XINS Isolated neutron stars with pulsed thermal X-ray emission but no detectable radio emission
MS Main-sequence star NS Neutron star CO CO or ONeMg White Dwarf He Helium White Dwarf UL Ultra-light companion or planet (mass < 0.08 solar masses) Note: If there is more than one companion, "T" (for Triple) is appended to the companion type. The innermost companion determines the type.