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    • 2. 发明公开
    • PARTICLE-OPTICAL APPARATUS INCLUDING A LOW-TEMPERATURE SPECIMEN HOLDER
    • 包含低温样品保持器的粒子光学装置
    • EP0901686A2
    • 1999-03-17
    • EP97913390.0
    • 1997-12-08
    • Koninklijke Philips Electronics N.V.
    • BORMANS, Bernardus, Jacobus, MarieDE JONG, Alan, FrankVAN DER MAST, Karel, DiederickWAGNER, RaymondASSELBERGS, Peter, Emile, Stephan, Joseph
    • G01Q30H01J37
    • H01J37/20H01J2237/2001
    • In an electron microscope it is sometimes important that specimens can be studied at a very low temperature (for example, that of liquid helium). In the case of known specimen holders the specimen is cooled by supplying the cooling medium via a bore in the specimen holder; this causes thermal drift of the removed specimen holder each time when a specimen is exchanged, and also an acoustic coupling (i.e. transfer of vibrations) exists with the dewar vessel connected to the specimen holder. In accordance with the invention, the specimen is arranged on the end (20) of the specimen holder (7) by means of a separate transport unit (13, 36) so that it is not necessary to remove the specimen holder (7) in order to exchange a specimen, with the result that the specimen holder is not heated. Moreover, the coupling to the cold source (22, 28) can take place via a flexible cooling conduit (30) which extends directly to the end (20) to be cooled and may be permanently connected thereto, thus avoiding the transfer of vibrations.
    • 在电子显微镜中,有时很重要的是样品可以在非常低的温度下进行研究(例如液氦)。 在已知样品夹具的情况下,通过经由样品夹具中的孔供应冷却介质来冷却样品; 这导致每次更换样本时被移除的样本架的热漂移,并且连接到样本架的杜瓦容器也存在声学耦合(即振动传递)。 根据本发明,通过单独的运输单元(13,36)将样本布置在样本保持器(7)的端部(20)上,使得不需要将样本保持器(7)移入 为了更换样本,导致样本架未被加热。 此外,与冷源(22,28)的连接可以通过直接延伸到待冷却的端部(20)的柔性冷却导管(30)进行并且可以与其永久连接,从而避免了振动的传递。
    • 4. 发明公开
    • PARTICLE-OPTICAL APPARATUS COMPRISING A FIXED DIAPHRAGM FOR THE MONOCHROMATOR FILTER
    • 包含用于单色滤光片的固定膜片的粒子光学装置
    • EP0795196A1
    • 1997-09-17
    • EP96930328.0
    • 1996-10-01
    • PHILIPS ELECTRONICS N.V.
    • TIEMEIJER, Peter, C.CHMELIK, JardaKRUIT, Pieter
    • H01J37
    • H01J37/05H01J2237/057
    • An electron microscope comprises an energy-selective filter (10) which is arranged ahead of the high-voltage field in the electron gun (2). Because the filter carries high-voltage potential and is arranged within the gun space (14) which is filled with SF6 gas, problems arise regarding electrical and mechanical passages to the filter. Notably the centering of the filter is problematic. In order to enable suitable aperture adjustment of the filter nevertheless (for current limitation and for avoiding optical aberrations introduced into the beam by the filter), there is provided an entrance diaphragm (30) which is rigidly connected to the filter parts, notably to a pole face or to a field-defining closing piece (48a) of the filter.
    • 电子显微镜包括布置在电子枪(2)的高压场之前的能量选择滤波器(10)。 因为滤波器承载高电压电势并且被布置在充满SF6气体的枪空间(14)内,所以关于到滤波器的电和机械通道出现问题。 值得注意的是过滤器的居中是有问题的。 然而,为了实现滤波器的合适的光圈调节(为了电流限制和为了避免由滤波器引入到光束中的光学像差),提供了刚性连接到滤波器部件的入射光阑(30),特别是与 极面或过滤器的场限定封闭件(48a)。
    • 7. 发明公开
    • METHOD FOR PARTICLE WAVE RECONSTRUCTION IN A PARTICLE-OPTICAL APPARATUS
    • METHOD FOR粒子波在粒子光学装置重建
    • EP0760109A1
    • 1997-03-05
    • EP96901465.0
    • 1996-02-15
    • Philips Electronics N.V.
    • COENE, Willem, Marie, JuliaJANSSEN, Augustus, Josephus, Elizabeth, Maria
    • G01Q60G01Q20G01Q30G02B7G02B21G03F7H01J37
    • G03F7/705H01J37/222H01J2237/223
    • A method for the iterative formation of an image of a specimen in a particle-optical apparatus. A series of experimental images (the experimental series) is recorded with each time a different setting of an imaging parameter (for example, the focal distance), and a comparable series of images is calculated on the basis of the electron wave at the specimen (the estimation). The two series are compared and on the basis thereof an electron wave is calculated (the feedback) with which a new series of images is calculated which better approximates the experimental series. This iteration step is repeated until the correspondence between the experimental series and the calculated series is sufficient, after which the asssociated electron wave is considered to be the desired image of the specimen. A subtantial gain as regards calculation time can be achieved during the estimation step as well as during the feedback step by executing the operation of the invention by means of FFTs. This is possible by writing the correlation expressions to be calculated in both steps in accordance with the invention in such a manner that they occur as pure correlation integrals which can be calculated by means of FFTs. The calculation time required when use is made of FFTs is substantially shorter than in the case of explicit calculation of the correlation expressions in conformity with the state of the art. The calculation time can thus be reduced by a factor of the order of magnitude of 50,000.