1887
banner image
No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
Optimal alignment control of a nonpolar molecule through nonresonant multiphoton transitions
Rent:
Rent this article for
USD
10.1063/1.3010369
/content/aip/journal/jcp/129/19/10.1063/1.3010369
http://aip.metastore.ingenta.com/content/aip/journal/jcp/129/19/10.1063/1.3010369
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

(a) Optimal pulse, (b) target expectation value , and (c) populations of rotational states as a function of time in the case of temperature . Time is measured in units of rotational period, (also see text). The control target is to maximize the degree of alignment at a specified final time, .

Image of FIG. 2.
FIG. 2.

Power spectrum of the optimal pulse in Fig. 1(a). The intensity is normalized to its highest peak. The frequency is measured in units of rotational constant . The inset shows the schematic illustration of optical transitions induced by the optimal pulse.

Image of FIG. 3.
FIG. 3.

(a) Optimal pulse, (b) target expectation value , and (c) populations of rotational states as a function of time in the case of temperature . The control target is to maximize the degree of alignment at a specified final time, . The optimal pulse is obtained from a different initial trial field from that in Fig. 1.

Image of FIG. 4.
FIG. 4.

Power spectrum of the optimal pulse in Fig. 3(a). The intensity is normalized to its highest peak. The frequency is measured in units of rotational constant . The inset shows the schematic illustration of optical transitions induced by the optimal pulse.

Image of FIG. 5.
FIG. 5.

(a) Optimal pulse and (b) target expectation value as a function of time in the case of temperature . The optimal pulse is obtained from the same initial trial field as that used in Fig. 3. The control target is to maximize the degree of alignment at a specified final time, . The time evolution of the population of each rotational state is shown in (c), (d), and (e), in which the initial conditions are , , and , respectively.

Image of FIG. 6.
FIG. 6.

(a) Optimal pulse, (b) target expectation value , and (c) populations of rotational states as a function of time in the case of temperature . The control target is to maintain the maximal degree of alignment over a specified time interval, (also see text).

Image of FIG. 7.
FIG. 7.

Power spectrum of the optimal pulse in Fig. 6(a). The intensity is normalized to its highest peak. The frequency is measured in units of rotational constant . The inset shows the schematic illustration of optical transitions induced by the optimal pulse.

Image of FIG. 8.
FIG. 8.

(a) Optimal pulse, (b) target expectation value , and (c) populations of rotational states as a function of time in the case of temperature . The control target is to maximize the degree of alignment at a specified final time, , in the presence of a given static field,

Image of FIG. 9.
FIG. 9.

Power spectrum of the optimal pulse in Fig. 8(a). The intensity is normalized to its highest peak. The frequency is measured in units of rotational constant . The inset shows the schematic illustration of optical transitions induced by the optimal pulse.

Loading

Article metrics loading...

/content/aip/journal/jcp/129/19/10.1063/1.3010369
2008-11-17
2014-04-18
Loading

Full text loading...

This is a required field
Please enter a valid email address
752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Optimal alignment control of a nonpolar molecule through nonresonant multiphoton transitions
http://aip.metastore.ingenta.com/content/aip/journal/jcp/129/19/10.1063/1.3010369
10.1063/1.3010369
SEARCH_EXPAND_ITEM