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  • American Society of Hematology  (63)
  • American Institute of Physics (AIP)  (42)
  • 1
    Publication Date: 2004-11-16
    Description: Rituximab proved to be effective in relapsed and refractory indolent NHL as a single agent and generated impressive results in phase II studies in combination with chemotherapy. In a prospective randomized trial we compared the efficacy and toxicity of rituximab (375 mg/m² d 1) plus MCP-chemotherapy ( mitoxantrone 8 mg/m² d 3 + 4, chlorambucile 3 x 3 mg/m² d 3 – 7, prednisolone 25 mg/m² d 3 – 7 ) given every 28 days for a total of 8 cycles versus MCP (d 1 – 5) x 8 cycles alone in advanced indolent NHL and MCL. Efficacy endpoints included overall and complete response rates, event free survival, progression free survival, overall survival and toxicity. For response assessment classical definitions have been used. Between 10/98 and 09/03 we randomized 358 patients (pts) with advanced stage follicular lymphoma (FL) (grade 1 + 2), lymphoplasmacytic lymphoma and MCL to either R-MCP or MCP. The study arms are well balanced for all demographic factors. 201/358 pts (56%) had FL. Both regimens were well tolerated with a low incidence of serious adverse events. The overall response rate (RR) and the complete response rate (CR) for all pts was 85,5% and 42% in the R-MCP arm versus 65,5% and 20% in the MCP arm (p
    Print ISSN: 0006-4971
    Electronic ISSN: 1528-0020
    Topics: Biology , Medicine
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  • 2
    Publication Date: 2004-11-16
    Description: Background: Clinical superiority of R-MCP (rituximab, mitoxantrone, chlorambucil, prednisolone) vs. MCP alone in patients with advanced stage indolent Non-Hodgkin’s-Lymphoma was demonstrated in a prospective, randomized, controlled, multicenter clinical trial (n=358). Data on resource utilization were collected alongside this clinical trial. Objective: To evaluate the health economic consequences, i.e. total cost and cost-consequences, of R-MCP vs. MCP from the perspective of a German payer (statutory sickness fund). Methods: Resource utilization data on 329 patients were collected and analyzed for the treatment phase (8 month). In addition, an interim analysis of the first 3 years of the subsequent observation period (planned: 7 years) was conducted. Data on resource utilization for initial chemotherapy, chemotherapy administration, treatment of adverse events, treatment of complications/progressive disease, subsequent chemotherapies and treatment for other reasons were collected. Several sensitivity analyses were performed to address different cost environments (e.g. treatment at university hospital vs. municipal hospital vs. private practice) and discounting scenarios. Results: Mean cost of the treatment phase in the base case analysis was EUR 35,890 for R-MCP (95%CI: EUR 33,178 – 38,602 and EUR 21,508 MCP per patient (95%CI: EUR 17,703 – 25,314). More treatment cycles were administered in the R-MCP arm (1,026 MCP, 1,237 R-MCP). Mean cost per active treatment cycle was EUR 4,932 for R-MCP (95%CI: EUR 4,512 – 5,353) and EUR 3,270 for MCP (95%CI: EUR 2,619 – 3,922). Mean (undiscounted) cost per patient in the observation period amounted to EUR 9,973 for R-MCP (95%CI: EUR 6,015 – 13,931) and EUR 15,896 for MCP (95%CI: 13,407 – 18,385). Mean observation time, after end of active treatment, was similar in both arms, 28.5 months for R-MCP, 27.5 months for MCP. Costs for treatment of adverse events, new chemotherapies and other reasons were reduced by 23%–39%, cost for treatment of progressive disease by 76% in the R-MCP arm compared to MCP alone. Extrapolating data to a full 3-year observation period results in savings of EUR 8,214 per patient with R-MCP compared to MCP alone. This compensates approx. 60% of the higher costs from the treatment phase. Clinically, R-MCP resulted in an objective response rate of 85.6% vs. 65.5% with MCP. After two years, based on Kaplan Maier estimate, event free survival for R-MCP was 69% vs. 44% for MCP alone (p〈 0.001) (For more detailed clinical results see abstract by Herold et al.) Conclusion: Initial treatment costs with R-MCP were EUR 14,382 higher compared to MCP alone. However, approx. 60% of additional costs are regained during the first three years after therapy due to savings for subsequent treatments, particularly for progressive disease. Combined with the clinical superiority of R-MCP, a favorable cost-effectiveness ratio may be expected when more mature data are available.
    Print ISSN: 0006-4971
    Electronic ISSN: 1528-0020
    Topics: Biology , Medicine
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  • 3
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The optimum conditions for the fabrication of semi-insulating InP epitaxial layers grown by metalorganic chemical-vapor deposition are investigated in a comparative study of the structural, electrical, and diffusive properties of Fe- and Ti-doped material. Thermally stable InP:Fe layers with resistivities approaching the intrinsic limit can be prepared in an environment of n-type material if the Fe concentration does not exceed but is close to its solubility limit of 8×1016 cm−3 at 640 °C. In contact with p-type layers, however, semi-insulating characteristics of InP:Fe turn out to be difficult to reproduce because of a pronounced interdiffusion of Fe and p-type dopants. Here, Ti doping of InP is shown to be a useful scheme for the fabrication of high-resistivity layers. New processes for the deposition of InP:Ti using (C5H5)2Ti(CO)2 and Ti[N(CH3)2]4 as metalorganic precursors are described in detail. Ti is found to compensate up to 2×1016 cm−3 of shallow acceptors in metalorganic chemical-vapor-phase-deposition-grown InP. Ti-doped InP layers containing more electrically active deep Ti donors than net shallow acceptors exhibit semi-insulating characteristics with a resistivity of 5×106 Ω cm. Codoping of InP:Fe with Ti turns out to be a universal process for the preparation of thermally stable high-resistivity layers. If the material is appropriately grown, Fe+Ti doping compensates both excess shallow donors and excess shallow acceptors up to concentrations of 8×1016 and 2×1016 cm−3, respectively. In contrast to InP:Fe, resistivities in excess of 107 Ω cm are obtained in contact with both symmetric n- and p-type current injecting contacts. Moreover, codoping of semi-insulating InP:Fe with Ti is found to suppress the interdiffusion of Fe and p-type dopants. Therefore, the outdiffusion and accumulation of Fe in other regions of complex device structures can be significantly reduced. The interdiffusion of Fe and p-type dopants as well as its suppression by additional doping with Ti, finally, is studied in detail, which enables a comprehensive model accounting for this phenomenon to be developed.
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 104 (1996), S. 8786-8794 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We have used composition depth profiling of polymer bilayers, based on nuclear reaction analysis, to determine miscibility, phase coexistence, and critical temperatures in mixtures of random olefinic copolymers of mean composition E1−x/EEx; here E is the ethylene group −(C4H8)−, EE is the ethylethylene group −[C2H3(C2H5)]−, and one of the copolymers is partially deuterated. The components in each binary mixture have different values x1,x2 of the EE fraction. Using a simple Flory–Huggins mixing model, our results enable us to extract an interaction parameter of the form χ(x1,x2,T)=A(x1,x2)/T, where for given x1,x2, A is a constant. Calculated binodals using this form fit our measured coexistence curves well, while allowing χ a weak composition dependence improves the fit further. Within the range of our parameters, our results suggest that in such binary polyolefin mixtures the interaction parameter increases roughly linearly with the extent of chemical mismatch expressed as the difference in degree of ethyl branching between the two components. © 1996 American Institute of Physics.
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 104 (1996), S. 8795-8806 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Using nuclear reaction analysis, we have measured the enrichment by one of the components at the surface of a binary mixture of random olefinic copolymers, with components of monomer structure E1−x1EEx1 and E1−x2EEx2. Here E and EE are the linear ethylene and branched ethylethylene groups (C4H8) and [C2H3(C2H5)], respectively, and x represents the fraction of the EE group randomly distributed on the chains. We examined 12 different couples covering a range x=0.38–0.97. The mixtures, whose thermodynamic behavior was established in our earlier paper, were cast in the form of films on both a silicon and on a gold-covered silicon surface, and were investigated in the one-phase region of the binodal in the vicinity of the critical temperature. We find that it is always the more flexible component—the one with a shorter statistical step length, corresponding to the higher ethylethylene fraction (higher x)—that is enriched at the polymer/air surface. Within our resolution neither component is enriched at the polymer/solid interface. These results show clearly that enthalpic rather than entropic factors dominate the surface potential driving the surface enrichment. For two of the mixtures we determined the excess of the surface-preferred species as a function of mixture composition along an isotherm in the one-phase region of the binodal. A consistent description of our data in terms of a mean-field model is provided by including in the surface potential a term in the mixture composition gradient at the polymer surface. © 1996 American Institute of Physics.
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  • 6
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: Energy dispersive x-ray spectroscopy of Kα transitions of neon and chlorine ions inside an electron cyclotron resonance (ECR) plasma is used to analyze the ion charge state distribution (CSD) inside the plasma. Basing on a computer code describing time dependent and stationary solutions of the balance equations for the CSD in ECR plasmas (considering single and multiple ionization and charge exchange processes, radiative recombination, vacancy cascades, and electron shake-off) and considering atomic properties (fluorescence yields, transition rates, x-ray energy shifts, x-ray production cross sections) of ions with different charge states, an approximation of simulated x-ray spectra to measured ones is possible. Thus the result we get is the corresponding CSD and information about the electron energy distribution function in the low energy region in the plasma. © 1998 American Institute of Physics.
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  • 7
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: Wavelength dispersive x-ray measurements on cobalt and krypton ions were presented to determine the ion charge state distribution (CSD) inside the electron cyclotron resonance (ECR) plasma of the 14.5 GHz ECR ion source of the TU Dresden. For clearly from the parent diagram lines separating x-ray satellites a comparison between calculated wavelength shifts and measured ones allows it to deduce the ion CSD of the analyzed ions. In the case of small line shifts (lower ionization states) a comparison with x-ray spectra derived from plasma modeling is done. By approximating the modeled spectra to the measured ones a most probable ion CSD was derived. © 1998 American Institute of Physics.
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  • 8
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: Energy dispersive x-ray spectroscopy of Kα transitions of neon and chlorine ions inside an electron cyclotron resonance (ECR) plasma is used to analyze the ion charge state distribution (CSD) inside the plasma. Basing on a computer code describing time dependent and stationary solutions of the balance equations for the CSD in ECR plasmas (considering single and multiple ionization and charge exchange processes, radiative recombination, vacancy cascades, and electron shake-off) and considering atomic properties (fluorescence yields, transition rates, x-ray energy shifts, x-ray production cross sections) of ions with different charge states, an approximation of simulated x-ray spectra to measured ones is possible. Thus the result we get is the corresponding CSD and information about the electron energy distribution function in the low energy region in the plasma. © 1998 American Institute of Physics.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 68 (1997), S. 4434-4438 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: The efficient confinement of the energetic charged fusion products and the complete transfer of their kinetic energy to the plasma is of great importance for the realization of a fusion reactor which will depend on alpha-particle heating. In todays fusion experiments with deuterium plasmas, this aspect can be investigated using the 1 MeV tritons from the d(d,p)t reaction. The slowing down behavior of these tritons can be studied by measuring the 14 MeV neutrons from the t(d,α)n reaction (triton burnup). At ASDEX Upgrade a time-resolved diagnostic based on a silicon barrier detector has been installed to measure the time evolution of the 14 MeV neutron rate. Using the Si(n,p)Al and Si (n,α)Mg reactions the high energy neutrons, with an energy above the 6 MeV threshold, are converted to charged particles directly inside the semiconductor diode. The complete functionality of the detector system is demonstrated by the successful measurement of the complex spectrum of the charged reaction products in silicon triggered by fusion neutrons during plasma discharges. As an integral component of this diagnostic a time dependent burnup code based on classical slowing-down theory has been developed for the use at ASDEX Upgrade to analyze the complex time evolution of the 14 MeV neutron rate. First measurements are compared to the results of the code. A new application for such detectors is proposed, as in conjunction with the materials of the tokamak structure it can be operated simultaneously as an in situ activation system. © 1997 American Institute of Physics.
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  • 10
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 69 (1998), S. 813-815 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: The metal ions from volatile compounds method was used to produce metal ion electron cyclotron resonance (ECR) plasmas and metal ion beams. In detail, the production of iron, nickel, and cobalt plasmas and beams on the 14.5 GHz ECR ion source of the TU Dresden is reported using ferrocene, nickelocene, and cobaltocene, respectively. Besides the detection of ion charge state distributions in extracted ion beams with an analyzing magnet first wavelength dispersive x-ray spectra of 3d cobalt metal ions were measured. Thereby, the based on atomic structure calculations analysis of x-ray satellites allows it to get information on the ion charge state spectrum of the ions inside the ECR plasma. © 1998 American Institute of Physics.
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