393 research outputs found

    The Canadian state and native migrant labour in southern Alberta's sugar beet industry

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    Recent studies of labour have clearly established that the capitalist state is very involved in the recruitment, relocation and retention of migrant labour forces. Most of the literature tends to analyze migrant labour within the broader social, political and economic context of expanding capitalism. Consequently, studies tend to focus on how the use of migrant labour is profitable to capitalism because it is cheap and easy to exploit. Such studies, however, neglect the ways in which the state actually intervenes in the labour market in order to facilitate the flow of migrant workers to places of employment. Therefore, this thesis explores the relationship between the migration of labour, the state and the reserve army of labour through an analysis of the Native migrant work force in the sugar beet industry in southern Alberta. Through the use of archival material, which includes various federal and provincial documents, annual reports of the Alberta Sugar Beet Growers' Association, newspapers and other materials, the circumstances underlying state intervention in the economy of the southern sugar beet industry became clear. While analyzing the structure of the sugar beet industry in southern Alberta, it was found that throughout much of the history of the sugar beet industry, farmers received low returns for their beet crops. Moreover, farmers also suffered financially from the high cost of machinery and, more recently, from the increased costs for fertilizer and chemical weed controls. An examination of government documents on the FederalProvincial Agricultural Manpower Committee, whose mandate was to recruit workers and move them to areas of need in agricultural sectors throughout Canada, revealed that the federal part of the committee was represented by officials from the Department of Manpower and Immigration and, beginning in the early 1950s, officials from the Department of Indian Affairs, who represented Indians on reserves. When the working conditions in sugar beet industry were examined, it was found that they were very poor for beet workers. In general, the weeding and hoeing of the sugar beets was difficult and the housing accommodations inadequate. Moreover, because of the low return on their beet crops and the high costs of machinery, fertilizer and weed control, the farmers had to keep the cost of labour as low as possible, which, meant paying low wages to beet workers. Moreover, it was found that throughout much the history of the sugar beet industry in southern Alberta, agricultural workers were unprotected by labour laws, which, was very conducive to reproducing conditions for cheap labour. Consequently, few wanted to work in the beet fields of southern Alberta if other employment could be found. Prior to the 1950s the state recruited immigrant workers and even prisoners of war from internment camps to supply farmers with the needed labour for their beet crops. However, in the early 1950s unskilled immigrant labour could no longer be procured for beet work. It was at this time that the sugar beet industry, through the Federal-Provincial Agricultural Manpower Committee, turned to recruiting Natives, particulary northern Alberta and northern Saskatchewan reserve Indians, to perform their labour requirements. In order to maintain this needed work force, the state helped organize Native migratation to southern Alberta at the start of the beet season and also helped ensure that they stayed there for the duration of the needed period

    PCN86 DRUG UTILIZATION AND COST CONSIDERATIONS OF ERYTHROPOIESIS-STIMULATING AGENTS (ESAS) IN PATIENTS WITH MYELODYSPLASTIC SYNDROMES (MDS)

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    Fermi-surface transformation across the pseudogap critical point of the cuprate superconductor La1.6x_{1.6-x}Nd0.4_{0.4}Srx_{x}CuO4_4

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    The electrical resistivity ρ\rho and Hall coefficient RH_H of the tetragonal single-layer cuprate Nd-LSCO were measured in magnetic fields up to H=37.5H = 37.5 T, large enough to access the normal state at T0T \to 0, for closely spaced dopings pp across the pseudogap critical point at p=0.235p^\star = 0.235. Below pp^\star, both coefficients exhibit an upturn at low temperature, which gets more pronounced with decreasing pp. Taken together, these upturns show that the normal-state carrier density nn at T=0T = 0 drops upon entering the pseudogap phase. Quantitatively, it goes from n=1+pn = 1 + p at p=0.24p = 0.24 to n=pn = p at p=0.20p = 0.20. By contrast, the mobility does not change appreciably, as revealed by the magneto-resistance. The transition has a width in doping and some internal structure, whereby RH_H responds more slowly than ρ\rho to the opening of the pseudogap. We attribute this difference to a Fermi surface that supports both hole-like and electron-like carriers in the interval 0.2<p<p0.2 < p < p^\star, with compensating contributions to RH_H. Our data are in excellent agreement with recent high-field data on YBCO and LSCO. The quantitative consistency across three different cuprates shows that a drop in carrier density from 1+p1 + p to pp is a universal signature of the pseudogap transition at T=0T=0. We discuss the implication of these findings for the nature of the pseudogap phase.Comment: 11 pages, 12 figure

    Isotropic three-dimensional gap in the iron-arsenide superconductor LiFeAs from directional heat transport measurements

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    The thermal conductivity k of the iron-arsenide superconductor LiFeAs (Tc ~ 18K) was measured in single crystals at temperatures down to T~50mK and in magnetic fields up to H=17T, very close to the upper critical field Hc2~18T. For both directions of the heat current, parallel and perpendicular to the tetragonal c-axis, a negligible residual linear term k/T is found as T ->0, revealing that there are no zero-energy quasiparticles in the superconducting state. The increase in k with magnetic field is the same for both current directions and it follows closely the dependence expected for an isotropic superconducting gap. There is no evidence of multi-band character, whereby the gap would be different on different Fermi-surface sheets. These findings show that the superconducting gap in LiFeAs is isotropic in 3D, without nodes or deep minima anywhere on the Fermi surface. Comparison with other iron-pnictide superconductors suggests that a nodeless isotropic gap is a common feature at optimal doping (maximal Tc).Comment: 4 pages, 3 figure

    Hall, Seebeck, and Nernst Coefficients of Underdoped HgBa2CuO4+d: Fermi-Surface Reconstruction in an Archetypal Cuprate Superconductor

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    Charge density-wave order has been observed in cuprate superconductors whose crystal structure breaks the square symmetry of the CuO2 planes, such as orthorhombic YBa2Cu3Oy (YBCO), but not so far in cuprates that preserve that symmetry, such as tetragonal HgBa2CuO4+d (Hg1201). We have measured the Hall (R_H), Seebeck (S), and Nernst coefficients of underdoped Hg1201 in magnetic fields large enough to suppress superconductivity. The high-field R_H(T) and S(T) are found to drop with decreasing temperature and become negative, as also observed in YBCO at comparable doping. In YBCO, the negative R_H and S are signatures of a small electron pocket caused by Fermi-surface reconstruction, attributed to charge density-wave modulations observed in the same range of doping and temperature. We deduce that a similar Fermi-surface reconstruction takes place in Hg1201, evidence that density-wave order exists in this material. A striking similarity is also found in the normal-state Nernst coefficient, further supporting this interpretation. Given the model nature of Hg1201, Fermi-surface reconstruction appears to be common to all hole-doped cuprates, suggesting that density-wave order is a fundamental property of these materials

    International Space Station Common Cabin Air Assembly Condensing Heat Exchanger Hydrophilic Coating Operation, Recovery, and Lessons Learned

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    The ability to control the temperature and humidity of an environment or habitat is critical for human survival. These factors are important to maintaining human health and comfort, as well as maintaining mechanical and electrical equipment in good working order to support the human and to accomplish mission objectives. The temperature and humidity of the International Space Station (ISS) United States On-orbit Segment (USOS) cabin air is controlled by the Common Cabin Air Assembly (CCAA). The CCAA consists of a fan, a condensing heat exchanger (CHX), an air/water separator, temperature and liquid sensors, and electrical controlling hardware and software. The CHX is the primary component responsible for control of temperature and humidity. The CCAA CHX contains a chemical coating that was developed to be hydrophilic and thus attract water from the humid influent air. This attraction forms the basis for water removal and therefore cabin humidity control. However, there have been several instances of CHX coatings becoming hydrophobic and repelling water. When this behavior is observed in an operational CHX in the ISS segments, the unit s ability to remove moisture from the air is compromised and the result is liquid water carryover into downstream ducting and systems. This water carryover can have detrimental effects on the ISS cabin atmosphere quality and on the health of downstream hardware. If the water carryover is severe and widespread, this behavior can result in an inability to maintain humidity levels in the USOS. This paper will describe the operation of the five CCAAs within the USOS, the potential causes of the hydrophobic condition, and the impacts of the resulting water carryover to downstream systems. It will describe the history of this behavior and the actual observed impacts to the ISS USOS. Information on mitigation steps to protect the health of future CHX hydrophilic coatings as well as remediation and recovery of the full heat exchanger will be discussed

    Combination therapy with rituximab, low-dose cyclophosphamide, and prednisone for idiopathic membranous nephropathy: a case series

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    BACKGROUND: Membranous nephropathy is a common cause of the nephrotic syndrome. Treatment with standard regimens fails to induce complete remission in most patients. We evaluated the efficacy of combination therapy with rituximab, low-dose, oral cyclophosphamide, and an accelerated prednisone taper (RCP) for the treatment of idiopathic membranous nephropathy. METHODS: We analyzed 15 consecutive patients with idiopathic membranous nephropathy treated with RCP at Massachusetts General Hospital. Seven patients (47%) received RCP as initial therapy, and the other eight patients (53%) received RCP for relapsing or refractory disease. All patients had at least 1 year of follow-up. The co-primary outcomes were attainment of partial and complete remission. Partial remission was defined as a urinary protein to creatinine ratio (UPCR) < 3 g/g and a 50% reduction from baseline. Complete remission was defined as a UPCR < 0.3 g/g. Secondary outcomes were serious adverse events and the change in proteinuria, serum creatinine, serum albumin, cholesterol, triglycerides, and immunoglobulin G levels after 1 year of treatment. RESULTS: Over a median follow-up time of 37 (IQR, 34-44) months, 100% of patients achieved partial remission and 93% of patients achieved complete remission at a median time of 2 and 13 months, respectively. After 1 year of treatment, median (IQR) UPCR declined from 8.2 (6.6-11.1) to 0.3 (0.2-0.7) g/g (P < 0.001). Three serious adverse events occurred over 51 patient years. No patients died or progressed to ESKD. CONCLUSIONS: Treatment of idiopathic membranous nephropathy with RCP resulted in high rates of complete remission. Larger studies evaluating this regimen are warranted

    Evidence for a small hole pocket in the Fermi surface of underdoped YBa2Cu3Oy

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    The Fermi surface of a metal is the fundamental basis from which its properties can be understood. In underdoped cuprate superconductors, the Fermi surface undergoes a reconstruction that produces a small electron pocket, but whether there is another, as yet undetected portion to the Fermi surface is unknown. Establishing the complete topology of the Fermi surface is key to identifying the mechanism responsible for its reconstruction. Here we report the discovery of a second Fermi pocket in underdoped YBa2Cu3Oy, detected as a small quantum oscillation frequency in the thermoelectric response and in the c-axis resistance. The field-angle dependence of the frequency demonstrates that it is a distinct Fermi surface and the normal-state thermopower requires it to be a hole pocket. A Fermi surface consisting of one electron pocket and two hole pockets with the measured areas and masses is consistent with a Fermi-surface reconstruction caused by the charge-density-wave order observed in YBa2Cu3Oy, provided other parts of the reconstructed Fermi surface are removed by a separate mechanism, possibly the pseudogap.Comment: 23 pages, 5 figure
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