PSR B0943+10 is known to show remarkably stable drifting subpulses, which can be interpreted in terms of a circumferential motion of 20 sparks, each completing one circulation around the periphery of the polar cap in 37 pulsar periods. We use this observational constraint and argue that the vacuum gap model can adequately describe the observed drift patterns. Further we demonstrate that only the presence of strong non-dipolar surface magnetic field can favor such vacuum gap formation. Subsequently, for the first time we are able to constrain the parameters of the surface magnetic field, and model the expected magnetic structure on the polar cap of PSR B0943+10 considering the inverse Compton scattering photon dominated vacuum gap
Aims.We examined a model of partially screened gap region above the polar cap, in which the electron...
A new drifting pulsar, PSR J0815+09, was discovered in the Arecibo drift-scan searches. An intriguin...
Current models of pulsar gamma-ray emission use the magnetic field of a rotating dipole in vacuum as...
PSR B0943+10 is known to show remarkably stable drifting subpulses, which can be interpreted in term...
In this paper we revisit the radio pulsar death line problem within the framework of curvature radia...
We propose vacuum gap (VG) model which can be applied uniformly for normal and high-magnetic-field p...
Despite the fact that pulsars have been observed for almost half a century, many questions have rema...
The classical vacuum gap model of Ruderman & Sutherland, in which spark-associated subbeams of subpu...
The analysis of X-ray observations suggest an ultrastrong ($B\gtrsim 10^{14} \,{\rm G}$) surface mag...
Recent work by Rankin & Deshpande strongly suggests that there exist strong "microstorms&qu...
We propose a vacuum gap (VG) model which can be applied uniformly for normal and high magnetic field...
A recent X-ray observation has shown that the radio pulsar PSR B0943 + 10, with clear drifting subpu...
The inner vacuum gap model has become the foundation stone of most theories on pulsar radio emission...
The classical vacuum gap model of Ruderman & Sutherland, in which spark-associated sub-beams of subp...
The unique and highly unusual drift feature reported for PSR J0815+0939, wherein one component's sub...
Aims.We examined a model of partially screened gap region above the polar cap, in which the electron...
A new drifting pulsar, PSR J0815+09, was discovered in the Arecibo drift-scan searches. An intriguin...
Current models of pulsar gamma-ray emission use the magnetic field of a rotating dipole in vacuum as...
PSR B0943+10 is known to show remarkably stable drifting subpulses, which can be interpreted in term...
In this paper we revisit the radio pulsar death line problem within the framework of curvature radia...
We propose vacuum gap (VG) model which can be applied uniformly for normal and high-magnetic-field p...
Despite the fact that pulsars have been observed for almost half a century, many questions have rema...
The classical vacuum gap model of Ruderman & Sutherland, in which spark-associated subbeams of subpu...
The analysis of X-ray observations suggest an ultrastrong ($B\gtrsim 10^{14} \,{\rm G}$) surface mag...
Recent work by Rankin & Deshpande strongly suggests that there exist strong "microstorms&qu...
We propose a vacuum gap (VG) model which can be applied uniformly for normal and high magnetic field...
A recent X-ray observation has shown that the radio pulsar PSR B0943 + 10, with clear drifting subpu...
The inner vacuum gap model has become the foundation stone of most theories on pulsar radio emission...
The classical vacuum gap model of Ruderman & Sutherland, in which spark-associated sub-beams of subp...
The unique and highly unusual drift feature reported for PSR J0815+0939, wherein one component's sub...
Aims.We examined a model of partially screened gap region above the polar cap, in which the electron...
A new drifting pulsar, PSR J0815+09, was discovered in the Arecibo drift-scan searches. An intriguin...
Current models of pulsar gamma-ray emission use the magnetic field of a rotating dipole in vacuum as...