101 research outputs found
The Anatomic Course of the First Jejunal Branch of the Superior Mesenteric Vein in Relation to the Superior Mesenteric Artery
Introduction. The purpose of this study is to determine the anatomic course of the first jejunal branch of the superior mesenteric vein (SMV) in relation to the superior mesenteric artery (SMA). Methods. Three hundred consecutive contrast-enhanced computed tomography (CT) scans were reviewed by a surgical oncologist with confirmation of findings by a radiologist. Results. The overall incidence of a first jejunal branch coursing anterior to the SMA was 41%. There was no correlation between patient gender and position of the jejunal branch. In addition, there was no correlation between size of the first jejunal branch and its location in relation to the SMA. The IMV drained into the SMV in 27% of the patients. The IMV drained into the SMV-portal vein confluence in 17% of patients and inserted into the splenic vein in 54%. An anterior coursing first jejunal branch statistically correlated with an IMV that drained into the SMV-portal vein confluence (P = 0.009). Conclusion. The first jejunal branch of the SMV has a highly variable course in relation to the SMA and has a higher incidence of an anterior location in this population than previously reported
Staging(18)F-FDG PET/CT influences the treatment plan in melanoma patients with satellite or in-transit metastases
Whole-body positron emission tomography/computed tomography (PET/CT) and brain magnetic resonance imaging (MRI) are commonly used to stage patients with palpable lymph node metastases from melanoma, but their role in patients with satellite and/or in-transit metastasis (S&ITM) is unclear. The aim of this study was to establish the diagnostic value of PET/CT and brain MRI in these patients, and to assess their influence on subsequent management decisions. In this prospective study, 25 melanoma patients with a first presentation of S&ITM who had no clinical evidence of palpable nodal or distant metastasis underwent whole-body(18)F-FDG PET/CT and brain MRI after a tentative pre-scan treatment plan had been made. Sensitivity and specificity of imaging were determined by pathological confirmation, clinical outcome and repeat PET/CT and MRI at 6 months. PET/CT led to a modification of the initial treatment plan in four patients (16%). All four were upstaged (AJCC stage eighth edition). PET/CT was false-positive in one patient, who had a Schwannoma in his trapezius muscle. A thyroid carcinoma was an incidental finding in another patient. The sensitivity of PET/CT was 58% and specificity 83%. In 6 months following the baseline PET/CT, further sites of in-transit or systemic disease were identified in 10 patients (40%). Brain MRI did not alter the treatment plan or change the disease stage in any patient. Whole-body PET/CT improved staging in melanoma patients with S&ITM and changed the originally-contemplated treatment plan in 16%. MRI of the brain appeared not to be useful
Quantum state preparation, tomography, and entanglement of mechanical oscillators
Precisely engineered mechanical oscillators keep time, filter signals, and
sense motion, making them an indispensable part of today's technological
landscape. These unique capabilities motivate bringing mechanical devices into
the quantum domain by interfacing them with engineered quantum circuits.
Proposals to combine microwave-frequency mechanical resonators with
superconducting devices suggest the possibility of powerful quantum acoustic
processors. Meanwhile, experiments in several mechanical systems have
demonstrated quantum state control and readout, phonon number resolution, and
phonon-mediated qubit-qubit interactions. Currently, these acoustic platforms
lack processors capable of controlling multiple mechanical oscillators' quantum
states with a single qubit, and the rapid quantum non-demolition measurements
of mechanical states needed for error correction. Here we use a superconducting
qubit to control and read out the quantum state of a pair of nanomechanical
resonators. Our device is capable of fast qubit-mechanics swap operations,
which we use to deterministically manipulate the mechanical states. By placing
the qubit into the strong dispersive regime with both mechanical resonators
simultaneously, we determine the resonators' phonon number distributions via
Ramsey measurements. Finally, we present quantum tomography of the prepared
nonclassical and entangled mechanical states. Our result represents a concrete
step toward feedback-based operation of a quantum acoustic processor.Comment: 13 pages, 4+5 figure
Coupling a superconducting quantum circuit to a phononic crystal defect cavity
Connecting nanoscale mechanical resonators to microwave quantum circuits
opens new avenues for storing, processing, and transmitting quantum
information. In this work, we couple a phononic crystal cavity to a tunable
superconducting quantum circuit. By fabricating a one-dimensional periodic
pattern in a thin film of lithium niobate and introducing a defect in this
artificial lattice, we localize a 6 gigahertz acoustic resonance to a
wavelength-scale volume of less than one cubic micron. The strong
piezoelectricity of lithium niobate efficiently couples the localized
vibrations to the electric field of a widely tunable high-impedance Josephson
junction array resonator. We measure a direct phonon-photon coupling rate
and a mechanical quality factor
leading to a cooperativity when
the two modes are tuned into resonance. Our work has direct application to
engineering hybrid quantum systems for microwave-to-optical conversion as well
as emerging architectures for quantum information processing.Comment: 9 pages, 7 figure
Quantum dynamics of a few-photon parametric oscillator
Modulating the frequency of a harmonic oscillator at nearly twice its natural
frequency leads to amplification and self-oscillation. Above the oscillation
threshold, the field settles into a coherent oscillating state with a
well-defined phase of either or . We demonstrate a quantum parametric
oscillator operating at microwave frequencies and drive it into oscillating
states containing only a few photons. The small number of photons present in
the system and the coherent nature of the nonlinearity prevents the environment
from learning the randomly chosen phase of the oscillator. This allows the
system to oscillate briefly in a quantum superposition of both phases at once -
effectively generating a nonclassical Schr\"{o}dinger's cat state. We
characterize the dynamics and states of the system by analyzing the output
field emitted by the oscillator and implementing quantum state tomography
suited for nonlinear resonators. By demonstrating a quantum parametric
oscillator and the requisite techniques for characterizing its quantum state,
we set the groundwork for new schemes of quantum and classical information
processing and extend the reach of these ubiquitous devices deep into the
quantum regime
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