V455 And
V515 And
AE Aqr
FO Aqr
V349 Aqr
XY Ari
V405 Aur
V647 Aur
HT Cam
MU Cam
DW Cnc
V709 Cas
V1025 Cen
V1033 Cas
TV Col
TX Col
UU Col
V2069 Cyg
V2306 Cyg
DO Dra
PQ Gem
V418 Gem
DQ Her
V1323 Her
V1460 Her
V1674 Her
EX Hya
NY Lup
V2400 Oph
V2731 Oph
V3037 Oph
V598 Peg
GK Per
AO Psc
HZ Pup
V667 Pup
WX Pyx
V1223 Sgr
V4743 Sgr
CC Scl
V1062 Tau
AX J1740.1
AX J1832.3
AX J1853.3
CTCV J2056
CXO J174954
IGR J04571
IGR J08390
IGR J15094
IGR J16500
IGR J16547
IGR J17014
IGR J17195
IGR J18151
IGR J18173
IGR J18308
IGR J19267
PBC J0927.8
PBC J1841.1
RX J1804
RX J2015
RX J2113
RX J2133
RX J2306
Swift J0717
Swift J1839
Swift J2006
Swift J2138

Full Catalog

Related Systems

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The Accretion Modes of IPs

The simplest picture of IPs is that they have a partial (and fully Keplerian) accretion disk, truncated by the magnetic field of the white dwarf. There is strong evidence of accretion disks (or at least disk-like structures) in many IPs (Hellier 1991). The X-ray orbital modulations seen in many IPs are also often (if not always) caused by azimuthal structure of the disk (Hellier, Garlick & Mason 1993; Parker, Norton & Mukai 2005).

The well known exception is V2400 Oph, which is usually thought to be a diskless accretor. That is, the primary's magnetic field is too strong to permit the formation of an accretion disk. X-ray modulations at one of two possible sidebands (\omega-\Omega or 2\omega-\Omega) are expected in diskless IPs (Wynn & King 1992), but not seen in most IPs (Hellier 1992).

There are three important numbers: the minimum distance between the ballistic trajectory from the L1 point and the white dwarf, rmin; the magnetospheric radius, rmag; and the circularization radius, rcir, where the specific angular momentum of the material in a Keplerian disk would equal that of the co-rotating material at the L1 point. A disk will definitely form if rmin > rmag, while a disk will definitely disappear if rmag > rcir. The case of rmin < rmag < rcir is tricky, since a disk should not be able to form but once formed, it can remain undisrupted. Since rmag is determined in part by the accretion rate, an episode of high accretion rate can establish a disk in this regime. Depending on the mass ratio of the binary, Pspin/Porb~0.1 corresponds to this regime.

This means that systems such as EX Hya are hard to understand in the standard, Keplerian, accretion disk picture. A series of papers based on the diamagnetic blob picture, however, explain such systems (Wynn & King 1995; Norton, Wynn & Somerscales 2004; Norton et al. 2008). The number of IPs for which such scenario is necessary has been increasing.

Then there is disk overflow accretion (Hellier 1993). For the overflow stream to directly accrete, something like this condition: rmin < rmag < rcir must be met.

In addition, a possibility that the partial disk may be misaligned with the orbital plane in IPs has been suggested.

Since this makes it a key parameter, we provide a table of confirmed IPs sorted by Pspin/Porb. We also show this graphically on the IP Home page.

References (General)

References (Specific Objects)

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Please send your comments, suggestions etc. to Koji.Mukai@nasa.gov and/or Koji.Mukai@umbc.edu
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