A beam intensity monitor for the Loma Linda cancer therapy proton accelerator

1991 ◽  
Vol 18 (4) ◽  
pp. 817-820 ◽  
Author(s):  
G. Coutrakon ◽  
Dan Miller ◽  
B. J. Kross ◽  
D. F. Anderson ◽  
P. DeLuca ◽  
...  
2011 ◽  
Vol 26 (10n11) ◽  
pp. 1852-1864 ◽  
Author(s):  
D. TRBOJEVIC ◽  
M. BLASKIEWICZ ◽  
E. FOREST

There are many possible applications for the non-scaling Fixed Field Alternating Gradient (NS-FFAG): accelerating non-relativistic ions, ion cancer therapy, proton drivers, accelerator driven subcritical reactors, heavy radioactive ions, recirculating linacs, and etc. They are confronted with two significant challenges: first is crossing integer resonances as the tunes vary with energy, and that the required fast acceleration has not yet been achieved in practice. An example of a small 30–250 MeV NS-FFAG proton accelerator is used to study both problems. After an introduction, the second chapter shows theoretical predictions for the emittance blow up from crossing the integer resonances. In the third part, the lattice of the ring is briefly described. The fourth chapter describes the "phase jump" a method for fast proton acceleration, while in the chapter five a six dimensional simulations of acceleration is described, ending with conclusions.


PEDIATRICS ◽  
1989 ◽  
Vol 84 (4) ◽  
pp. A37-A37

Last month, scientists at the Fermi National Accelerator Laboratory here unveiled the first proton beam accelerator built for hospital use. When the machine is ready for operation next year at Loma Linda University Medical Center near Los Angeles, many believe it will prove itself a major breakthrough in the wan on cancer. Others, however, think the proton accelerator is a white elephant. They complain that its untested medical benefits and enormous price make it the ultimate example of medical technology run amok. Some doctors say proton therapy will prove useless in the treatment of most cancers. It is unquestionably the most expensive piece of medical equipment ever built. The cost—$40 million, including the special building needed to house the machine—dwarfs the cost of the next most expensive medical device: the Positron Emitting Tomography scanner, which shows metabolic activity within the brain and can cost about $5 million. Protons were first suggested as a potential cancer therapy in 1946 by Robert Rathbun Wilson, who established the Fermi National Accelerator Laboratory. But it wasn't until the 1970s that patients were first exposed to protons in physics labs at Harvard University, the University of California at Berkeley, at Fermi and at several institutions abroad. In physics labs cluttered with cable and oscilloscopes, physicists have seen some spectacular results using physics research machines moonlighting to treat cancer patients. At Harvard, where 174 patients with malignant tumors at the base of the brain have been treated, the therapy has had an 85% cure rate, compared with 35% cure rate for conventional therapies. (Patients in remission or cancer-free for five years are considered cured.) The beam is virtually useless in cancers that have spread beyond the original site. Such metastacized (sic) cancers account for more [than] two thirds of all malignancies says [one] radiation oncologist. "There's some usefulness, no doubt about it. But the candidates for proton therapy are limited. . . . It won't make a major impact on the cure rates for all cancers. It will make a little dent, but it will cost a lot to make that dent.


Author(s):  
A. Yamaguchi ◽  
K. Nakayama ◽  
T. Rizawa ◽  
S. Sukenobu ◽  
K. Satoh ◽  
...  

Laser Physics ◽  
2006 ◽  
Vol 16 (4) ◽  
pp. 639-646 ◽  
Author(s):  
C. -M. Ma ◽  
I. Veltchev ◽  
E. Fourkal ◽  
J. S. Li ◽  
W. Luo ◽  
...  

Author(s):  
S. S. Sheinin ◽  
C. D. Cann

The effects of systematic reflections on the variation of diffracted beam intensity with depth in a crystal can only be taken into account by using the multi-beam dynamical theory. The results of calculations of this kind, which are presented here, indicate that the intensity profiles obtained are not periodic. Since extinction distance is a concept strictly applicable only when the diffracted beam intensity varies periodically with depth, its use as a parameter in describing multi-beam intensity profiles must be carefully considered.


Author(s):  
JR Fryer ◽  
Z Huang ◽  
D Stirling ◽  
G. Webb

Platinum dispersed on γ-alumina is used as a reforming catalyst to convert linear hydrocarbons to cyclic aromatic products. To improve selectivity and lifetime of the catalyst, other elements are included, and we have studied the distributions of Pt/Re, and Pt/Sn, bimetallic systems on the support both before and after use in octane reforming. Often, one or both of the components are not resolvable by HREM or microanalysis as individual particles because of small size and lack of contrast on the alumina, and divergent beam microanalysis has been used to establish the presence and relationship between the two elements.In the majority of catalysts the platinum is in the form of small panicles, some of which are large enough to be resolvable in the microscope. The ABT002B microscope with Link windowless Pentafet detector, used in this work, was able to obtain a resolvable signal from particles of 2nm diameter upwards. When the beam was concentrated on to such a particle the signal was at a maximum, and as the beam diameter was diverged - at the same total beam intensity and dead time - the signal decreased as shown in Figure 1.


2021 ◽  
Author(s):  
Jintong Liu ◽  
Jing Huang ◽  
Lei Zhang ◽  
Jianping Lei

We review the general principle of the design and functional modulation of nanoscaled MOF heterostructures, and biomedical applications in enhanced therapy.


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