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1.
Appl Radiat Isot ; 61(4): 547-50, 2004 Oct.
Artigo em Inglês | MEDLINE | ID: mdl-15246397

RESUMO

In this paper, we will discuss a phase-contrast imaging method that avoids the complications of interferometry to provide phase contrast in weakly absorbing samples. A transversely coherent neutron beam is used with the traditional radiography scheme. Images taken with this scheme show dramatic intensity variations due to sharp changes in the neutron wave refractive index. With some numerical processing these images may be used to reconstruct a quantitative phase radiograph of specimens imaged with this technique.

2.
J Microsc ; 214(Pt 1): 62-9, 2004 Apr.
Artigo em Inglês | MEDLINE | ID: mdl-15049869

RESUMO

The ability to image phase distributions with high spatial resolution is a key capability of microscopy systems. Consequently, the development and use of phase microscopy has been an important aspect of microscopy research and development. Most phase microscopy is based on a form of interference. Some phase imaging techniques, such as differential interference microscopy or phase microscopy, have a low coherence requirement, which enables high-resolution imaging but in effect prevents the acquisition of quantitative phase information. These techniques are therefore used mainly for phase visualization. On the other hand, interference microscopy and holography are able to yield quantitative phase measurements but cannot offer the highest resolution. A new approach to phase microscopy, quantitative phase-amplitude microscopy (QPAM) has recently been proposed that relies on observing the manner in which intensity images change with small defocuses and using these intensity changes to recover the phase. The method is easily understood when an object is thin, meaning its thickness is much less than the depth of field of the imaging system. However, in practice, objects will not often be thin, leading to the question of what precisely is being measured when QPAM is applied to a thick object. The optical transfer function formalism previously developed uses three-dimensional (3D) optical transfer functions under the Born approximation. In this paper we use the 3D optical transfer function approach of Streibl not for the analysis of 3D imaging methods, such as tomography, but rather for the problem of analysing 2D phase images of thick objects. We go on to test the theoretical predictions experimentally. The two are found to be in excellent agreement and we show that the 3D imaging properties of QPAM can be reliably predicted using the optical transfer function formalism.


Assuntos
Eritrócitos/ultraestrutura , Imageamento Tridimensional/métodos , Microscopia de Contraste de Fase/métodos , Animais , Células Cultivadas , Humanos , Processamento de Imagem Assistida por Computador/métodos , Modelos Teóricos , Miócitos de Músculo Liso/ultraestrutura , Ratos
3.
Phys Rev Lett ; 91(14): 145502, 2003 Oct 03.
Artigo em Inglês | MEDLINE | ID: mdl-14611534

RESUMO

We develop and experimentally demonstrate a formalism that allows accurate phase imaging using neutron sources producing highly polychromatic beams. The results of measurements from a rectangular block of silicon compare favorably with theoretical simulations based upon the known composition and geometry of the block. The increased flux and reduced exposure times will permit a simple extension of the technique to tomographic phase imaging.

4.
J Microsc ; 206(Pt 3): 204-8, 2002 Jun.
Artigo em Inglês | MEDLINE | ID: mdl-12067364

RESUMO

Although phase contrast microscopy is widespread in optical microscopy, it has not been as widely adopted in transmission electron microscopy (TEM), which has therefore to a large extent relied on staining techniques to yield sufficient contrast. Those methods of phase contrast that are used in biological electron microscopy have been limited by factors such as the need for small phase shifts in very thin samples, the requirement for difficult experimental conditions, or the use of complex data analysis methods. We here demonstrate a simple method for quantitative TEM phase microscopy that is suitable for large phase shifts and requires only two images. We present a TEM phase image of unstained Radula sp. (liverwort spore). We show how the image may be transformed into the differential interference contrast image format familiar from optical microscopy. The phase images contain features not visible with the other imaging modalities. The resulting technique should permit phase contrast TEM to be performed almost as readily as phase contrast optical microscopy.


Assuntos
Microscopia Eletrônica/métodos , Microscopia de Interferência/métodos , Microscopia de Contraste de Fase/métodos , Animais , Células Eucarióticas/ultraestrutura , Microscopia de Contraste de Fase/instrumentação , Esporos/ultraestrutura
6.
J Opt Soc Am A Opt Image Sci Vis ; 17(10): 1732-43, 2000 Oct.
Artigo em Inglês | MEDLINE | ID: mdl-11028521

RESUMO

We demonstrate quantitative noninterferometric x-ray phase-amplitude measurement. We present results from two experimental geometries. The first geometry uses x rays diverging from a point source to produce high-resolution holograms of submicrometer-sized objects. The measured phase of the projected image agrees with the geometrically determined phase to within +/-7%. The second geometry uses a direct imaging microscope setup that allows the formation of a magnified image with a zone-plate lens. Here a direct measure of the object phase is made and agrees with that of the magnified object to better than +/-10%. In both cases the accuracy of the phase is limited by the pixel resolution.

7.
Appl Opt ; 33(10): 1806-11, 1994 Apr 01.
Artigo em Inglês | MEDLINE | ID: mdl-20885511

RESUMO

A method is presented for the experimental determination of refractive-index profiles for planar media of monotonically decreasing refractive index, such as those used for optical waveguides. The technique is based on a generalization of the classical experiment of Lloyd's mirror, involving the interference pattern formed by a point source and its mirage, i.e., its reflection in such a graded planar medium.

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