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Biomedical subjects

J C Hill

Publications and source records attributed to J C Hill.

At least 19 recordsLinked to original sources

Truncal adiposity is present at birth and in early childhood in South Indian children.

OBJECTIVES: Muscle-thin but adipose ('thin-fat') body composition of south Asian adults contributes to their high risk of type 2 diabetes. Studies in Pune, India showed that this phenotype is present at birth. We aimed to determine if south Indian babies have a 'thin-fat' phenotype and if this persists in childhood. DESIGN: Prospective cohort study. SETTING: Holdsworth Memorial Hospital, Mysore, India. SUBJECTS: Children (n = 663) whose mothers were recruited from the antenatal clinics. METHODS: Weight, length, head, mid-upper-arm, abdominal circumferences; triceps and subscapular skinfolds were measured at birth, one and four years, and compared with white Caucasian babies born in Southampton, UK (birth), and UK and Dutch growth standards (one and four years). RESULTS: Mysore babies were lighter (2983 g vs 3472 g; -1.10 SD, CI -1.16, -1.02) and smaller in all body measurements than UK neonates (P < 0.001). The deficit was greatest for mid-upper-arm (-1.07 SD), head (-0.89 SD) and abdominal circumferences (-0.73 SD), and least for length (-0.25 SD) and subscapular skinfold thickness (-0.19 SD). Predictors of skinfold thickness were maternal body mass index (P < 0.001) and socio-economic status (P = 0.05). At four years, subscapular skinfold thickness was larger than UK (+0.18 SD, CI +0.11, +0.25; P < 0.001) and Dutch standards (+0.61 SD, CI +0.51, +0.71; P < 0.001), despite all other body measurements remaining smaller. Predictors of 4-year skinfold thickness were neonatal skinfold thickness (P = 0.001) and maternal insulin concentrations (P = 0.05). CONCLUSIONS: Mysore newborns have a 'thin-fat' phenotype. This may reflect the action of genes and/or the 'maternal environment'. The phenotype persists in childhood, and may be the forerunner of a diabetogenic adult phenotype.

Abdomen↗

Flow measurements via two-particle azimuthal correlations in Au + Au collisions at sqrt [s(NN)]=130 GeV.

Two-particle azimuthal correlation functions are presented for charged hadrons produced in Au+Au collisions at the Relativistic Heavy Ion Collider (sqrt [s(NN)]=130 GeV). The measurements permit determination of elliptic flow without event-by-event estimation of the reaction plane. The extracted elliptic flow values (v2) show significant sensitivity to both the collision centrality and the transverse momenta of emitted hadrons, suggesting rapid thermalization and relatively strong velocity fields. When scaled by the eccentricity of the collision zone epsilon, the scaled elliptic flow shows little or no dependence on centrality for charged hadrons with relatively low p(T). A breakdown of this epsilon scaling is observed for charged hadrons with pT >1.0 GeV/c.

Journal Article↗

Measurement of Lambda and Lambda(macro) particles in Au+Au collisions at the square root of S(NN) = 130 GeV.

We present results on the measurement of Lambda and Lambda(macro) production in Au+Au collisions at square root of (S (NN) = 130 GeV with the PHENIX detector at the Relativistic Heavy Ion Collider. The transverse momentum spectra were measured for minimum bias and for the 5% most central events. The Lambda;/Lambda ratios are constant as a function of p(T) and the number of participants. The measured net Lambda density is significantly larger than predicted by models based on hadronic strings (e.g., HIJING) but in approximate agreement with models which include the gluon-junction mechanism.

Journal Article↗

Net charge fluctuations in Au + Au interactions at sqrt[s(NN)]=130 GeV.

Data from Au + Au interactions at sqrt[s(NN)]=130 GeV, obtained with the PHENIX detector at the Relativistic Heavy-Ion Collider, are used to investigate local net charge fluctuations among particles produced near midrapidity. According to recent suggestions, such fluctuations may carry information from the quark-gluon plasma. This analysis shows that the fluctuations are dominated by a stochastic distribution of particles, but are also sensitive to other effects, like global charge conservation and resonance decays.

Journal Article↗

Centrality dependence of pi(+/-), K(+/-), p, and (-)p production from sqrt[s(NN)] = 130 GeV Au + Au collisions at RHIC.

Identified pi(+/-), K(+/-), p, and (-)p transverse momentum spectra at midrapidity in sqrt[s(NN)] = 130 GeV Au+Au collisions were measured by the PHENIX experiment at RHIC as a function of collision centrality. Average transverse momenta increase with the number of participating nucleons in a similar way for all particle species. Within errors, all midrapidity particle yields per participant are found to be increasing with the number of participating nucleons. There is an indication that K(+/-), p, and (-)p yields per participant increase faster than the pi(+/-) yields. In central collisions at high transverse momenta (p(T) > or =2 GeV/c), (-)p and p yields are comparable to the pi(+/-) yields.

Journal Article↗

Transverse-mass dependence of two-pion correlations in Au+Au collisions at square root[s(NN)] = 130 GeV.

Two-pion correlations in square root[s(NN)] = 130 GeV Au+Au collisions at RHIC have been measured over a broad range of pair transverse momentum k(T) by the PHENIX experiment at RHIC. The k(T) dependent transverse radii are similar to results from heavy-ion collisions at square root[s(NN)] = 4.1, 4.9, and 17.3 GeV, whereas the longitudinal radius increases monotonically with beam energy. The ratio of the outwards to sidewards transverse radii (R(out)/R(side)) is consistent with unity and independent of k(T).

Journal Article↗

Measurement of single electrons and implications for charm production in Au+Au collisions at square root[s(NN)] = 130 GeV.

Transverse momentum spectra of electrons from Au+Au collisions at square root[s(NN)] = 130 GeV have been measured at midrapidity by the PHENIX experiment at the Relativistic Heavy Ion Collider. The spectra show an excess above the background from photon conversions and light hadron decays. The electron signal is consistent with that expected from semileptonic decays of charm. The yield of the electron signal dN(e)/dy for p(T) > 0.8 GeV/c is 0.025+/-0.004(stat)+/-0.010(syst) in central collisions, and the corresponding charm cross section is 380+/-60(stat)+/-200(syst) microb per binary nucleon-nucleon collision.

Journal Article↗

Disappearance of intraperitoneal gas following gynaecological laparoscopy.

We investigated 25 day case gynaecological laparoscopy patients to determine the duration of the pneumoperitoneum, the rate at which residual gas disappeared and the relative contribution of this gas to pain in the early postoperative period. The volume of gas was calculated from measurements of the subdiaphragmatic gas bubble obtained from an erect chest X-ray. Each patient was X-rayed twice, either immediately prior to discharge and at 24 h post laparoscopy, or at 24 h and 48 h post surgery. Patients were contacted by telephone at 24 and 48 h to confirm fitness to return for the X-ray and at the same time verbal pain and activity scores were recorded. We found that residual gas was almost entirely gone by 48 h following surgery and that it appeared to reduce in an exponential manner. The contribution of this gas to postoperative pain was significant in the first 24 h, but by 48 h it was considerably reduced. We conclude that in day case gynaecological laparoscopy patients, postoperative pneumoperitoneum is short-lived, and that by 48 h its volume and contribution to postoperative pain should be minimal.

Ambulatory Surgical Procedures↗

Suppression of hadrons with large transverse momentum in central Au+Au collisions at root square[s(NN)] = 130 GeV.

Transverse momentum spectra for charged hadrons and for neutral pions in the range 1 GeV/c<p(T)<5 GeV/c have been measured by the PHENIX experiment at RHIC in Au+Au collisions at root square[s(NN)] = 130 GeV. At high p(T) the spectra from peripheral nuclear collisions are consistent with scaling the spectra from p+p collisions by the average number of binary nucleon-nucleon collisions. The spectra from central collisions are significantly suppressed when compared to the binary-scaled p+p expectation, and also when compared to similarly binary-scaled peripheral collisions, indicating a novel nuclear-medium effect in central nuclear collisions at RHIC energies.

Journal Article↗

Measurement of the midrapidity transverse energy distribution from square root of [(s)NN] = 130 GeV Au + Au collisions at RHIC.

The first measurement of energy produced transverse to the beam direction at the Relativistic Heavy-Ion Collider at Brookhaven National Laboratory is presented. The midrapidity transverse energy density per participating nucleon rises steadily with the number of participants, closely paralleling the rise in charged-particle density, such that / remains relatively constant as a function of centrality. The energy density calculated via Bjorken's prescription for the 2% most central Au+Au collisions at square root[s(NN)] = 130 GeV is at least epsilon(Bj) = 4.6 GeV/fm(3), which is a factor of 1.6 larger than found at sqrt[s(NN)] = 17.2 GeV ( Pb+Pb at CERN).

Journal Article↗

Centrality dependence of charged particle multiplicity in Au-Au collisions at square root of (s)NN = 130 GeV.

We present results for the charged-particle multiplicity distribution at midrapidity in Au-Au collisions at square root of [s(NN)] = 130 GeV measured with the PHENIX detector at RHIC. For the 5% most central collisions we find dN(ch)/d eta(vertical line eta = 0) = 622+/-1(stat)+/-41(syst). The results, analyzed as a function of centrality, show a steady rise of the particle density per participating nucleon with centrality.

Journal Article↗

Patterns of abnormal FDG uptake by various histological types of non-small cell lung cancer at initial staging by PET.

The aim of this study was to identify useful patterns of abnormal fluorine-18 fluorodeoxyglucose (FDG) uptake by different types of non-small cell (NSC) lung cancer and to assess their clinical implications. One hundred and three sequential patients with newly diagnosed, pathology-proven NSC lung cancer were included. FDG positron emission tomography (PET) images were acquired using a dedicated PET scanner. There were 35 squamous cell carcinomas (SQC), 17 large cell cancers (LGC), 38 adenocarcinomas (ADC), 1 bronchioloalveolar carcinoma (BAC) and 12 non-classified NSC cancers. PET images were categorized into detectable patterns of necrotic center in the primary tumor, satellite lesions (T4), hilar lymph nodes (N1), and N2, N3, and M1 lesions by visual interpretation of PET images for SQC, LGC, and ADC (n=90; BAC and non-classified NSC cancers were excluded). The PET lesions were correlated with surgical pathology and with CT findings in inoperable cases. Necrosis was more commonly present in the primary tumors of LGC (53%) and SQC (43%) than in those of ADC (26%) (P<0.0001 and <0.01, respectively). The frequencies of nodal uptake in ADC, SQC and LGC were similar (71%, 60%, and 59%, respectively). However, M1 lesions were present significantly more often in LGC (41%) and ADC (34%) than in SQC (3%) (both P<0.0001). Significantly more surgically inoperable cases were found by PET (T4, N3, M1) in ADC (50%) and LGC (41%) than in SQC (26%) (P<0.001 and <0.02, respectively). Our results suggest a wide variation of PET findings for different types of NSC lung cancer. Identification of these patterns is useful in clinical PET interpretation, in that knowledge of the most probable association between the PET patterns and the histological types will facilitate initial staging and planning of management.

Adenocarcinoma↗

Malignant melanoma of the eyelid and palpebral conjunctiva treated with iodine-125 brachytherapy.

OBJECTIVE: To evaluate the results on malignant melanomas of the eyelid and palpebral conjunctiva treated with iodine-125 (125I) brachytherapy with shielding of the eye. DESIGN: Noncomparative case series. PARTICIPANTS: Fourteen patients treated with 125I brachytherapy at an ocular oncology referral center from 1974 through 1996, all of whom had had previous debulking, incomplete resection, or recurrence after surgery. INTERVENTION: A stainless steel pericorneal ring eyeshield was attached to the extraocular muscles, over which a lid was fitted to protect the cornea without touching it. Iodine-125 seeds in polythene tubes were inserted into the eyelid and attached to the lid margin for a single plane implant. In five cases additional seeds were glued on to the shield as well for a volume implant. A median dose of 37 Gy (range, 17.3-67.6 Gy) was given over the course of 113 hours (range, 47-190 hours) to the outer surface of target volume. MAIN OUTCOME MEASURES: Local control is regarded as freedom from recurrence in those without measurable disease and complete clinical regression in those with measurable disease. Morbidity is assessed in terms of function and cosmesis. Survival is given from the time of the implant. RESULTS: There was local control in 13 patients maintained from 11 to 227 months (median, 39 months). There were two recurrences at 8 and 13 months in the first patient who received 17.3 Gy. Late complications consisted of mild eyelid telangiectasia, mild eyelid atrophy, and loss of eyelashes in most patients. Five patients, four of whom had upper eyelid tumors, experienced a dry eye, which was managed with tear supplements, and one of these patients developed a cataract. A corneal ulcer developed in one eye, which later perforated after treatment of a subsequent bulbar melanoma and was exenterated. Another eye was enucleated after treatment for a subsequent melanoma in the fornix. Cosmesis was acceptable to patient and doctor in the other 12 patients. Vision was maintained in seven patients, reduced in two, and not recorded in the remaining three patients. Three patients died of hematogenous metastases at 44, 62, and 79 months after implant, one of bronchial carcinoma at 46 months and one of an astrocytoma at 39 months. All patients were clear of local disease. The remainder survived for a median of 45 months (range, 18-227 months). CONCLUSIONS: Iodine-125 brachytherapy can be used as an alternative to wide excision or exenteration of these tumors. There was good local control, reasonable maintenance of vision, and good cosmesis.

Adult↗

Impact of radionuclide ventriculography prior to elective abdominal aortic reconstruction.

We evaluated how preoperative radionuclide ventriculography (RNV) influences the clinical management of 96 patients referred for elective infrarenal abdominal aortic surgery. Of these, 11 had aortoiliac occlusive disease and 85 an abdominal aortic aneurysm. In 89 patients (93%), there was a known history or clinical evidence of coronary artery disease prior to RNV. The scan was abnormal in half the patients. There were 56 patients with left ventricular ejection fraction (LVEF) > 50% and 40 with LVEF < or = 50%. The LVEF ranged between 10% and 88% with a mean of 52.8+/-14.1%. There was normal wall motion in 56 patients and wall abnormalities were present in 40, including four LV aneurysms. After initial assessment, 19 patients did not proceed to surgery for a variety of reasons. Cardiology consultation was requested in 11 patients, six of which were delayed or turned down for surgery mainly on cardiac grounds. Only one of these underwent cardiac catheterization. Of the remaining 77 patients who underwent surgery, 15 were seen by a cardiologist and one was delayed in order to optimize his cardiac status. No patient underwent prophylactic coronary angioplasty/stenting or revascularization preoperatively. In addition, based on the RNV results and in conjunction with the clinical findings, six patients had pulmonary artery catheters inserted either the night prior to operation (n = 3) or after induction to anaesthesia (n = 3). This is the largest reported British series of cardiac testing using RNV prior to abdominal aortic surgery. Coronaryartery disease is very common amongst such patients. RNV influences our decision-making and patientselection. An abnormal result may alter the clinical management, lead to a cardiology referral (26/96, 27% in this series) and have anaesthetic implications.

Aged↗

HLA-A and -B alleles in cornea donors as risk factors for graft rejection.

We determined the human leucocyte antigen (HLA)-A, -B and -DR allele frequencies in recipients and donors of 115 cornea transplants, for recipients who developed graft rejection and those who did not. No difference in HLA allele frequencies of the recipients was found. The frequencies of the HLA-A26, -B35 and -B44 alleles in cornea donors were increased in recipients who developed graft failure. The detrimental effect on corneal graft survival of these alleles was significant (p < 0.001). No such effect was observed in renal transplantation. Corneal graft survival was similar when one or two A26, B35 or B44 alleles were present on the donor cornea. The negative effect was similar in magnitude to the previously reported negative effect of an HLA-B locus match between donor and recipient. When both a B-locus match and an A26, B35 or B44 allele were present, the negative effect on graft survival was twice as strong, indicating that different immune mechanisms are responsible for these phenomena.

Alleles↗