Method for the production of wideband THz radiation
Abstract
A method for the production of extremely wide bandwidth THz radiation comprising: delivering an electron beam from a source to an undulator that does not deflect the angle or transversely move the electron beam; and optimizing the undulator to yield peak emission in the middle of the THz band (1 THz). These objectives are accomplished by magnetically bending the orbit of the incoming electron beam in the undulator according to the function x(z)=x.sub.o exp(-z.sup.2/2.sigma..sup.2) and controlling the transverse magnetic field to be B(z)=B.sub.0(1-z.sup.2/.sigma..sup.2)exp(-z.sup.2/2.sigma..sup.2).
- Inventors:
-
- Newport News, VA
- Issue Date:
- Research Org.:
- Southeastern Universities Research Association
- Sponsoring Org.:
- USDOE
- OSTI Identifier:
- 921632
- Patent Number(s):
- 7315141
- Application Number:
- 11/204,536
- Assignee:
- Jefferson Science Associates LLC (Newport News, VA)
- Patent Classifications (CPCs):
-
H - ELECTRICITY H05 - ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR H05H - PLASMA TECHNIQUE
- DOE Contract Number:
- AC05-84ER40150
- Resource Type:
- Patent
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 07 ISOTOPE AND RADIATION SOURCES
Citation Formats
Krafft, Geoffrey A. Method for the production of wideband THz radiation. United States: N. p., 2008.
Web.
Krafft, Geoffrey A. Method for the production of wideband THz radiation. United States.
Krafft, Geoffrey A. Tue .
"Method for the production of wideband THz radiation". United States. https://www.osti.gov/servlets/purl/921632.
@article{osti_921632,
title = {Method for the production of wideband THz radiation},
author = {Krafft, Geoffrey A},
abstractNote = {A method for the production of extremely wide bandwidth THz radiation comprising: delivering an electron beam from a source to an undulator that does not deflect the angle or transversely move the electron beam; and optimizing the undulator to yield peak emission in the middle of the THz band (1 THz). These objectives are accomplished by magnetically bending the orbit of the incoming electron beam in the undulator according to the function x(z)=x.sub.o exp(-z.sup.2/2.sigma..sup.2) and controlling the transverse magnetic field to be B(z)=B.sub.0(1-z.sup.2/.sigma..sup.2)exp(-z.sup.2/2.sigma..sup.2).},
doi = {},
journal = {},
number = ,
volume = ,
place = {United States},
year = {2008},
month = {1}
}