Zobrazeno 1 - 10
of 38
pro vyhledávání: '"Mirko I Hrovat"'
Autor:
James P. Butler, Alan Hrovat, Feng Zhou, Mirko I. Hrovat, Iga Muradyan, Samuel Patz, C. Corey Hardin, Angelos Kyriazis, Mikayel Dabaghyan, Eric Frederick
Publikováno v:
NMR in Biomedicine. 27:1479-1489
In this work, we report initial results from a light-weight, low field magnetic resonance device designed to make relative pulmonary density measurements at the bedside. The development of this device necessarily involves special considerations for t
Autor:
Kyle J. McInnis, Steven K. Grinspoon, Samantha G. Harrington, Meaghan A. McCarthy, Loredana Farilla, Bijoy J. Thomas, Shana E. McCormack, Martin Torriani, Mirko I. Hrovat, Amy Fleischman, David M. Systrom
Publikováno v:
Pediatric Obesity. 9:281-291
Background Obesity is associated with poor fitness and adverse metabolic consequences in children.
Autor:
Loredana Farilla, Amy Fleischman, Steven K. Grinspoon, Meaghan A. McCarthy, Shana E. McCormack, David M. Systrom, Mirko I. Hrovat
Publikováno v:
The Journal of Clinical Endocrinology & Metabolism. 96:E1612-E1618
Periods of rapid growth require an increase in energy use and substrate formation. Mitochondrial function contributes to each of these and therefore may play a role in longitudinal growth.Twenty-nine children and adolescents of ages 8-15 yr were enro
Publikováno v:
Magnetic Resonance in Medicine. 60:1433-1443
The density of the organic matrix of bone substance is a critical parameter necessary to clinically evaluate and distinguish structural and metabolic pathological conditions such as osteomalacia in adults and rickets in growing children. Water and fa
Autor:
Iga Muradian, Stephen Ketel, Samuel Patz, Iulian C. Ruset, Mirko I. Hrovat, Francine L. Jacobson, George P. Topulos, F. William Hersman, James P. Butler, Hiroto Hatabu
Publikováno v:
European Journal of Radiology. 64:335-344
The majority of researchers investigating hyperpolarized gas MRI as a candidate functional lung imaging modality have used (3)He as their imaging agent of choice rather than (129)Xe. This preference has been predominantly due to, (3)He providing stro
Autor:
Walter R. Frontera, Christian T. Farrar, David M. Systrom, Steven K. Grinspoon, Mirko I. Hrovat, Kathleen V. Fitch, Bijoy J. Thomas, Martin Torriani, Stine Johnsen, Hélène C. F. Côté, Amy Fleischman
Publikováno v:
American Journal of Physiology-Endocrinology and Metabolism. 292:E1666-E1673
Mitochondrial dysfunction may contribute to the development of insulin resistance and type 2 diabetes. Nucleoside reverse transcriptase inhibitors (NRTIs), specifically stavudine, are known to alter mitochondrial function in human immunodeficiency vi
Autor:
Samuel Patz, George P. Topulos, Ronald L. Walsworth, James P. Butler, Mirko I. Hrovat, Matthew S. Rosen, F. W. Hersman, Leo L. Tsai, J. Ng, I. Muradian, Iulian C. Ruset, Ross W. Mair
Publikováno v:
Concepts in Magnetic Resonance Part B: Magnetic Resonance Engineering. :210-221
We describe a prototype system built to allow open-access very-low-field MRI of human lungs using laser-polarized (3)He gas. The system employs an open four-coil electromagnet with an operational B(0) field of 4 mT, and planar gradient coils that gen
Autor:
Yuly M. Pulyer, Mirko I. Hrovat
Publikováno v:
Journal of Magnetic Resonance. 154:298-302
Ferro-refraction is the field magnification that is obtained when a current segment is near a high magnetic permeable boundary. It is shown that ferro-refraction may be used in the design of magnets for NMR or MRI to increase the efficiency of these
Analytic reconstruction of magnetic resonance imaging signal obtained from a periodic encoding field
Publikováno v:
Medical Physics. 27:2060-2064
We have proposed a two-dimensional PERiodic-Linear (PERL) magnetic encoding field geometry B(x,y) = g(y)y cos(q(x)x) and a magnetic resonance imaging pulse sequence which incorporates two fields to image a two-dimensional spin density: a standard lin
Publikováno v:
International Journal of Imaging Systems and Technology. 10:216-224
A new magnetic field geometry for spatial encoding of magnetic resonance imaging (MRI) is presented. The field is given by: Bz(x, y) = gyy cos(qxx), and is called a PERL field because it is PERiodic in x and Linear in y. Both imaging pulse sequences