High-Energy Isolated Attosecond Pulses

Author(s):  
M. Lucchini ◽  
F. Ferrari ◽  
F. Calegari ◽  
C. Vozzi ◽  
S. Stagira ◽  
...  
2020 ◽  
Vol 117 (20) ◽  
pp. 10727-10732
Author(s):  
Yu-Chen Cheng ◽  
Sara Mikaelsson ◽  
Saikat Nandi ◽  
Lisa Rämisch ◽  
Chen Guo ◽  
...  

When small quantum systems, atoms or molecules, absorb a high-energy photon, electrons are emitted with a well-defined energy and a highly symmetric angular distribution, ruled by energy quantization and parity conservation. These rules are based on approximations and symmetries which may break down when atoms are exposed to ultrashort and intense optical pulses. This raises the question of their universality for the simplest case of the photoelectric effect. Here we investigate photoionization of helium by a sequence of attosecond pulses in the presence of a weak infrared laser field. We continuously control the energy of the photoelectrons and introduce an asymmetry in their emission direction, at variance with the idealized rules mentioned above. This control, made possible by the extreme temporal confinement of the light–matter interaction, opens a road in attosecond science, namely, the manipulation of ultrafast processes with a tailored sequence of attosecond pulses.


2012 ◽  
Vol 45 (7) ◽  
pp. 074018 ◽  
Author(s):  
E Constant ◽  
A Dubrouil ◽  
O Hort ◽  
S Petit ◽  
D Descamps ◽  
...  

Author(s):  
Francesca Calegari ◽  
Federico Ferrari ◽  
Matteo Lucchini ◽  
Caterina Vozzi ◽  
Salvatore Stagira ◽  
...  

Author(s):  
Daniel E. Rivas ◽  
Matthew Weidman ◽  
Boris Bergues ◽  
Alexander Muschet ◽  
Alexander Guggenmos ◽  
...  

2010 ◽  
Vol 4 (12) ◽  
pp. 875-879 ◽  
Author(s):  
F. Ferrari ◽  
F. Calegari ◽  
M. Lucchini ◽  
C. Vozzi ◽  
S. Stagira ◽  
...  

2006 ◽  
Vol 349 (1-4) ◽  
pp. 256-263 ◽  
Author(s):  
Alexander S. Pirozhkov ◽  
Sergei V. Bulanov ◽  
Timur Zh. Esirkepov ◽  
Michiaki Mori ◽  
Akito Sagisaka ◽  
...  

1984 ◽  
Vol 75 ◽  
pp. 599-602
Author(s):  
T.V. Johnson ◽  
G.E. Morfill ◽  
E. Grun

A number of lines of evidence suggest that the particles making up the E-ring are small, on the order of a few microns or less in size (Terrile and Tokunaga, 1980, BAAS; Pang et al., 1982 Saturn meeting; Tucson, AZ). This suggests that a variety of electromagnetic and plasma affects may be important in considering the history of such particles. We have shown (Morfill et al., 1982, J. Geophys. Res., in press) that plasma drags forces from the corotating plasma will rapidly evolve E-ring particle orbits to increasing distance from Saturn until a point is reached where radiation drag forces acting to decrease orbital radius balance this outward acceleration. This occurs at approximately Rhea's orbit, although the exact value is subject to many uncertainties. The time scale for plasma drag to move particles from Enceladus' orbit to the outer E-ring is ~104yr. A variety of effects also act to remove particles, primarily sputtering by both high energy charged particles (Cheng et al., 1982, J. Geophys. Res., in press) and corotating plasma (Morfill et al., 1982). The time scale for sputtering away one micron particles is also short, 102 - 10 yrs. Thus the detailed particle density profile in the E-ring is set by a competition between orbit evolution and particle removal. The high density region near Enceladus' orbit may result from the sputtering yeild of corotating ions being less than unity at this radius (e.g. Eviatar et al., 1982, Saturn meeting). In any case, an active source of E-ring material is required if the feature is not very ephemeral - Enceladus itself, with its geologically recent surface, appears still to be the best candidate for the ultimate source of E-ring material.


Author(s):  
J. B. Warren

Electron diffraction intensity profiles have been used extensively in studies of polycrystalline and amorphous thin films. In previous work, diffraction intensity profiles were quantitized either by mechanically scanning the photographic emulsion with a densitometer or by using deflection coils to scan the diffraction pattern over a stationary detector. Such methods tend to be slow, and the intensities must still be converted from analog to digital form for quantitative analysis. The Instrumentation Division at Brookhaven has designed and constructed a electron diffractometer, based on a silicon photodiode array, that overcomes these disadvantages. The instrument is compact (Fig. 1), can be used with any unmodified electron microscope, and acquires the data in a form immediately accessible by microcomputer.Major components include a RETICON 1024 element photodiode array for the de tector, an Analog Devices MAS-1202 analog digital converter and a Digital Equipment LSI 11/2 microcomputer. The photodiode array cannot detect high energy electrons without damage so an f/1.4 lens is used to focus the phosphor screen image of the diffraction pattern on to the photodiode array.


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