Closed Koalaaaaaa closed 2 years ago
Yes, the Laser
block's omega
should be equal to 1, while the reference frequency in the Main
block equal to reference_angular_frequency_SI=2*math.pi*c/L
, where L
and c
are in m
and m/s
respectively.
but when I read the literature, they always define the pulse frequency as 50kHz or 25kHz, so I'm really confused. I have another question, after the first pulse, would the electron and ion recombined? When I shoot the second pulse after the electron density tend to be stable, the density doesn't change any more. It seems like un physical.
In this case for example https://www.osapublishing.org/abstract.cfm?uri=ASSL-2021-ATh3A.4 50 kHz is the repetition rate of the ultraviolet laser. So they are multiple ultraviolet pulses shot with a frequency of 50 kHz. But since they are ultraviolet, the carrier frequency of the pulses will be in the ultraviolet range. Can it be also your case?
so the smilei code identifies the light is in the range of EUV by the wr I difined. Got it, thank your sir. emmmm, when I define the spatial and temprol resolution according to the debye length and plasma frequency, my simulation should last at least for 20us. There is an error about Segment error (core dumped). When I decrease the simulation time, no error. I don't know if it is because I just use a normal laptop without MPI. really thanks for your helps in this two days.
In this case for example https://www.osapublishing.org/abstract.cfm?uri=ASSL-2021-ATh3A.4 50 kHz is the repetition rate of the ultraviolet laser. So they are multiple ultraviolet pulses shot with a frequency of 50 kHz. But since they are ultraviolet, the carrier frequency of the pulses will be in the ultraviolet range. Can it be also your case?
oh I think the 50kHz I should define in the time_envelope
In the time_envelope
you should define the temporal profile of the single pulse, not the whole train of pulses. Physically a ultraviolet laser with 50 kHz repetition rate is given by a sequence of pulses with carrier frequency in the ultraviolet range, the distance between the pulses given by c/50kHz~6e3 m. This distance is enormous, you don't simulate the train of pulses.
Instead, with this repetition rate you typically simulate the effect of the single pulse. If each pulse is a gaussian, then in the time_envelope
you should put this gaussian profile. Note that in this case you have three characteristic lengths:
time_envelope
in the Laser
block.Main
block.Please use Issues to ask questions, to report bugs or for feature requests only after you have a clear idea of what you want to simulate. The chat room is more suited for this kind of questions.
The segmentation fault is likely related to the CFL condition. Check if you have a warning
hello everyone and happy new year! In my simulation, a beam of extreme ultra-violet shoot into the box and ionize the background low pressure hydrogen. So I choose the tunnel ionization model to simulate the process of ionization, I do not know if it is right. For the EUV whose wave length is L = 13.5nm, so the frequency is w = c/L, so I defined the reference frequency as wr = 2piw. In the Laser block , the omega = 1 (unit in wr). Does it right? Thanks for your help and best wishes!