
Supplier: Airbus Group
Description: Airbus Defence and Space heritage in supply of Solid State Power Amplifiers (SSPAs) for satellite applications spans more than 20 years. Much of that heritage is founded on products in L and S bands but this has now been extended to cover the C band 3.7GHz to 4.2GHz. This linearised C Band SSPA
 Product Category: Power Amplifier / SSPA
 Frequency: 3.70E9 to 4.20E9 Hz
 Gain: 70 dB
 Operating Temperature: 22 to 167 F

Supplier: Evertz Microsystems Ltd.
Description: The XRF1A is an RF signal routing matrix for LBand and IF satellite communications and other signals. Housed in a compact 1RU chassis and available in 8x8 or 16x16 matrix sizes, the XRF1A is a fullfeatured routing matrix with automatic or manual gain control and RF power meters on each input

Supplier: TMP Pro Distribution
Description: of dedicated record outputs that makes it easier to create a stereo recording of the mix. The console also features an output matrix with seven feeds to four outputs, being fed from the group busses and main L, R and C (mono) outputs. The GB4 offers a comprehensive set of functions and facilities in a small

Supplier: Nivelco USA
Description: FEATURES :: Twowire TDR Technology Digital communication High accuracy: Â±5 mm High pressure range High temperature range Extremely low dead band Large DotMatrix graphic display Local programming feature Textbased menu system Plastic coated stainless steel probes (PFA, FEP
 Media Type: Liquid, Dry Material (Bulk Solids and Powders)
 Level Measurement Type: Continuous Level
 Output Options: Analog Current Signal (e.g., 420 mA)
 Measuring Range: 11.81 to 945 inch

Supplier: Visual Sound, Inc.
Description: Midas Consoles The Midas XL42 is a 1U rack mounted, dual channel creative equaliser incorporating the XL4 fourband parametric equalisation with XL4 mic/line preamplifiers and 48V phantom supply. Each channel has input, output and pan rotary controls, 10 segment LED metering plus a switchable
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Poloidaltoroidal decomposition in a finite cylinder. II.
Discretization, regularization and validation
With f and g represented in the polynomial radial basis (2.8), a recursion relation exists for r2H, as stated in section 2.1, i.e. r2H = R−1L with R, L banded matrices .

Computational Structural Analysis and Finite Element Methods
Then order the unnumbered members of the stars of the nodes in the selected sequence, to obtain a reasonably banded L matrix .

ZAMM �? Journal of Applied Mathematics and Mechanics
A similar approach reduces the bandwidth of C. Simplified algorithm: Order the nodes of S and order the unnumbered edges of the stars of the nodes in the selected sequence, to obtain a reasonably banded L matrix .

Scaling of the spin stiffness in random spin chains
Hence, using this notation, we can rewrite the Hamiltonian (7) in terms of a symmetric L × L band ma trix A(φ) as .

Crossover effects in the random exchange spin1/2 antiferromagnetic
chain
works;5,14,16,31 it amounts to a numerical calculation of the eigenvectors of a L × L band matrix and then the evaluation of a (r −1)×(r −1) (resp. 2 ×2) determinant 10 .

Darboux transforms on Band Matrices, Weights and associated Polynomials
...207, pp. 589620 (1999), we have shown that mperiodic sequences of weights lead to �?moments�?, polynomi als defined by determinants of matrices involving these moments and 2m+1step relations between them, thus leading to 2m + 1 band matrices L .

Distributing the Kalman Filter for LargeScale Systems
2We refer to a matrix as an L banded matrix ( L ≥ 0), if the elements outside the band defined by the Lth upper and Lth lower diagonal are 0.

Cooperation for aggregating complex electric power networks to ensure system observability
1We refer to a matrix as an L banded matrix ( L ≥ 0), if the elements outside the band defined by the Lth upper and Lth lower diagonal are 0.

Model Distribution for Distributed Kalman Filters: A Graph Theoretic Approach
3We refer to a matrix as an L banded matrix ( L > 0), if the elements outside the band defined by the Lth upper and Lth lower diagonal are zero. to sensor 1 are F(1) and D(1), as shown in (15).

Numerical Mathematics
Program 11  forwband : Forward substitution for a banded matrix L .

Integrable discrete hungry systems and their related matrix eigenvalues
Not only the band matrices L (n) + dI appearing in Sect.

The discrete hungry Lotka–Volterra system and a new algorithm for computing matrix eigenvalues
In the band matrix L (n) of the Lax form shown . in section 2, as n → ∞, the entry U(n) Mk converges to the positive constant ck and the other converges to zero where c1 . c2 .

Vector Stieltjes Continued Fraction and Vector QD Algorithm
in l2 (N) by the biinfinite band matrix L , whose elements Li,i+1 = 1 and Li−p,i = ai are the only nonzero entries, for any p .

Isospectral deformations of general matrix and their reductions on Lie algebras
The generalized Toda equation with band matrix L .

Ramanscattering results on transformations in finely divided titanium dioxide
as the 480 cm  l matrix band narrows and the anatase line vanishes, while the rutile lines strengthen (curves 4 and 5).