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Process for bulk alternating copolymerization of propylene

1. A process for bulk alternating 100, wherein R1, R2, and R3, are the same monovalent aliphatic hydrocarbon radical with 4 to

ISOPRENE OR BUTADIENE CIS 1,4-POLYMERIC BI-COMPONENT CATALYST

Complex 4: R1 = 2,6-(CH2CH3)2-C6H3, 1-100:1; when the alkylating reagent is an isoprene or butadiene monomers is bulk

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Devices formed utilizing organic materials

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Cu2ZnSnS4 as a New Solar Cell Material: The History and the

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A Review on the Properties of Iron Aluminide Intermetallics

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Conjugated polymers provided with at least one MIP and a

(7) according to any of claims 1 to 4, bulk material in accordance with an embodiment of In embodiments according to the invention, R1

Low-resolution data analysis for low-density lipoprotein

bulk solvent (protein and phospholipid head groups100.0 100.0 100.0 100.0 99.5 100.0 94.r1 = (0, 0, 1/4) and the symmetry-related

Method for producing a functional, high-energy material

high-energetic material with layered grain 1 to 4, characterized in that a diffusion depth with R1=C1-C10-alkyl, C1-C10-alkoxy or aryl

A new process chain for producing bulk metallic glass

bulk metallic glasses (BMG) to achieve the (2010) Some recent advances in multi-material Int J Adv Manuf Technol 47(1–4):161–180

Shortcuts for graviton propagation in a six-dimensional brane

0.4 0.6 0.8 t 1 Figure 2: Shortcuts for in six-dimensional AdS- Schwarzschild bulk. two hori- zons if and only if h(r1) ≤ 0

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Bulk fields with brane terms

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The inhomogeneous jet parameters in active galactic nuclei

information on the bulk motions of the emitting so one has to assume that the VLBI observing hundred, which is mainly due to extremely low

Warped Phenomenology of Higher-Derivative Gravity

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Reservoir characterization and improved oil recovery from

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produced with anionic dyes on cellulose fibre material

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Modeling the Broadband Emission of GRB 090902B

100 MeV) up to 103 s after the burst, and general Online-only material: color figures 1. Adopting R = 4γ 2cT , the bulk Lorentz

Fast radiation mediated shocks and supernova shock breakouts

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STRANGELETS IN COSMIC RAYS

charge aSections 1 and 2 are partly based on and extrinsic curvature C = 1 R1 + 1 R2 dSbulk radius per baryon as (13) R0 = (3/4π