Abstract: The present invention relates to a process for preparing 1,2-propanediol by hydrogenation of glycerol by means of hydrogen gas, wherein glycerol is reacted with hydrogen in at least “i” fluidically interconnected reactors R1 to Ri each having a hydrogenation catalyst to form 1,2-propanediol, wherein the process comprises sequential steps from reactors R1 through Rn, wherein n as used hereinafter is an integer in the range from 2 to i. The process includes introducing hydrogen gas and a glycerol phase into the first reactor R1 and a first 1,2-propanediol containing phase and a first hydrogen phase are formed in the reactor, and introducing sequentially the 1,2-propanediol containing phase formed in the preceding reactor and hydrogen into each of the subsequent reactors wherein the glycerol phase containing at least 60% by weight, based on the total weight of the glycerol phase of glycerol.

Abstract: A method is disclosed for the operation of a high-power electron beam for the vaporization of materials in a target. With this method, static and dynamic deflection errors are corrected. First, the static and dynamic deflection errors are ascertained by means of a teach-in process for concrete spatial coordinates and concrete frequencies of the deflection currents and stored in a memory. For the later operation, this stored data is used in such a way that input geometric data for the incidence points of the electron beam is automatically recalculated into corrected current values which bring about the exact incidence onto the input points. A corresponding procedure takes place with the input of frequencies for the deflection current. The input frequencies are automatically corrected in terms of frequency and amplitude in order to eliminate the frequency-dependent attenuation effects.

Abstract: A method is disclosed for the operation of a high-power electron beam for the vaporization of materials in a target. With this method, static and dynamic deflection errors are corrected. First, the static and dynamic deflection errors are ascertained by means of a teach-in process for concrete spatial coordinates and concrete frequencies of the deflection currents and stored in a memory. For the later operation, this stored data is used in such a way that input geometric data for the incidence points of the electron beam is automatically recalculated into corrected current values which bring about the exact incidence onto the input points. A corresponding procedure takes place with the input of frequencies for the deflection current. The input frequencies are automatically corrected in terms of frequency and amplitude in order to eliminate the frequency-dependent attenuation effects.

Abstract: A method is disclosed for the operation of a high-power electron beam for the vaporization of materials in a target. With this method, static and dynamic deflection errors are corrected. First, the static and dynamic deflection errors are ascertained by means of a teach-in process for concrete spatial coordinates and concrete frequencies of the deflection currents and stored in a memory. For the later operation, this stored data is used in such a way that input geometric data for the incidence points of the electron beam is automatically recalculated into corrected current values which bring about the exact incidence onto the input points. A corresponding procedure takes place with the input of frequencies for the deflection current. The input frequencies are automatically corrected in terms of frequency and amplitude in order to eliminate the frequency-dependent attenuation effects.

Abstract: A sputtering cathode with a flat plate-shaped target (8) and a tub-shaped yoke (3) arranged behind the target (8), with center ridge (5) and with magnets (7,7′) for generating an enclosed tunnel of arc-shaped curved field lines (15,15′) in front of the target surface, as well as with three sheet metal cutouts (9,10,11) or groups of partial cutouts inserted into the plane between the target (8) and the end faces (12) of the tub rim of the yoke (3) facing the target (8), all the sheet metal cutouts (9,10,11) together form two gaps (a,b) extending roughly parallel to the end faces (12,13), wherein the magnets (7,7′) are each incorporated or inserted into the yoke bottom and the side surfaces of the magnets (7,7′) facing towards and away from the target (8) run flush with the yoke bottom.

Abstract: In a sputter cathode with a plate-shaped target (8) and with a trough-shaped yoke (3), arranged behind the target (8), with middle web (5) and with magnets (7, 7', . . . ) for producing a closed tunnel of field lines (15, 15', . . . ) curved in an arc in front of the target surface as well as with three sheet-metal blanks (9, 10, 11) consisting of one layer of a compound plate e.g. of an aluminum/iron compound plate, which blanks are placed into the plane between the target (8) and the front surfaces (12, 13) of the trough edge of the yoke (3), which front surfaces face the target (8), all sheet-metal blanks (9, 10, 11) of magnetically conductive material together form gaps (a, a') extending approximately parallel to the front surfaces (12, 13), which gaps (a, a') are filled out between the sheet-metal blanks (9, 10, 11) by the other layer (21) of the compound plate.

Abstract: A vacuum coating device coats substrates on all sides by rotating the substrates in a material flow. The device is for use in a vacuum chamber with a material source, and includes a holder for holding the substrates opposite the material source and drives correlated with the holder to bring about a rotation and shifting movement of the substrates. The device includes a hollow manipulator arm formed from three legs which extend at an angle with respect to one another. More specifically, the first leg extends at an obtuse angle with respect to the second leg, and the second leg extends at an approximately right-angle with respect to the third leg. The substrates are then held at the end of the third leg by the holder. The manipulator arm, when driven by a motor, can rotate around the longitudinal axis of the first leg, and, moreover, can move back and forth in the direction of this longitudinal axis.

Abstract: Pole shoes (3, 4, 5) of magnetically conductive material are provided inside of a first tubular target (2). Outside the target (2), a magnetic flux guide element (7) is provided, which has three pole shoes (8, 9, 10) directed toward the hollow body (1), which are connected to each other by magnets (12, 13). These magnets (12, 13) transmit the magnetic field through the target (2) to the pole shoes (3, 4, 5) inside the target (2) across narrow gaps (6, 11).

Abstract: A magnetic deflection system for a high-power electron beam with an expanding cross-section area is used for melting or vaporizing metallic materials. Saddle coils are provided which open in a direction of expansion of the electron beam. With the aid of these saddle coils large deflection speeds of the electron beam are obtained with small imaging errors and large deflection angles.