Results 141 to 150 of about 600 (183)
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Hyperfunctions in one variable, hyperfunctions in the Nilsson class
2011Hyperfunctions in one variable. Differentiation of a hyperfunction. The local nature of the notion of a hyperfunction. The integral of a hyperfunction. Hyperfunctions whose support is reduced to a point. Hyperfunctions in the Nilsson class.
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Steroids, 1995
To elucidate the mechanisms of abnormal steroid production in hyperfunctioning and non-hyperfunctioning adrenal tumors, we examined both the activities and amounts of steroidogenic cytochromes P450 in the tumor and non-tumor portions of these adrenals at the posttranslational (protein) level.
H, Suzuki +4 more
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To elucidate the mechanisms of abnormal steroid production in hyperfunctioning and non-hyperfunctioning adrenal tumors, we examined both the activities and amounts of steroidogenic cytochromes P450 in the tumor and non-tumor portions of these adrenals at the posttranslational (protein) level.
H, Suzuki +4 more
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Thyroid Hyperfunction During Pregnancy
Thyroid, 1998The present report focuses on the two main causes of hyperthyroidism observed in the pregnant state: Graves' disease (GD) and gestational transient thyrotoxicosis. Together, the prevalence of hyperthyroidism may represent 3% to 4% of all pregnancies, and therefore constitutes an important clinical issue. Concerning GD, the variable presentations of the
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1992
Let D be a domain containing a part or the whole of the x-axis. Denote the parts of D above and below the x-axis by D+ and D− respectively. Let F +(z) be an analytic function regular in D+ and F −(z) an analytic function regular in D−. If the limit f(x) defined by $$f(x) = \mathop {\lim }\limits_{ \in \to + 0} \{ {F_ + }(x + i \in ) - {F_ - }(x - i
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Let D be a domain containing a part or the whole of the x-axis. Denote the parts of D above and below the x-axis by D+ and D− respectively. Let F +(z) be an analytic function regular in D+ and F −(z) an analytic function regular in D−. If the limit f(x) defined by $$f(x) = \mathop {\lim }\limits_{ \in \to + 0} \{ {F_ + }(x + i \in ) - {F_ - }(x - i
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Introduction to Hyperfunctions
2010After a short overview of generalized functions and of the different ways they can be defined, the concept of a hyperfunction is established, followed by an introduction to the most simple and familiar hyperfunctions. Then the elementary operational properties of hyperfunctions are presented.
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HYPERFUNCTION AND HYPOFUNCTION IN THE ANTERIOR PITUITARY
Nursing Clinics of North America, 1996The actions and interactions of the pituitary gland and the nervous system constitute a regulatory system whereby the physiologic activity of the thyroid, adrenals, and gonads is controlled. Damage to or interference with the pituitary gland may cause hyper- or hypofunctional states resulting in devastating changes in a person's body and life.
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1992
Our aim is to construct hyperfunctions so that they have as close a relation as possible to ordinary functions. Of the operations of addition, subtraction, multiplication and division, the first two are, of course, possible as linear combinations. There are, however, problems with multiplication and division.
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Our aim is to construct hyperfunctions so that they have as close a relation as possible to ordinary functions. Of the operations of addition, subtraction, multiplication and division, the first two are, of course, possible as linear combinations. There are, however, problems with multiplication and division.
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The Hyperfunctioning Thyroid Nodule
Southern Medical Journal, 1969W M, Morton, J W, Runyan
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1992
Let us begin with two ordinary functions φ 1(x) and φ 2(x) and suppose that their Fourier transforms $${\psi _1}(\xi ) = F{\phi _1}(x),{\psi _2}(\xi ) = F{\phi _2}(x)$$ (1.1) exist. The Fourier transform of the product φ 1(x) · φ 2(x) is $$F\{ {\phi _1}(x){\phi _2}(x)\} = {\text{ }}\int_{ - \infty }^\infty {{\phi _1}(x){\phi _2}(x){e ...
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Let us begin with two ordinary functions φ 1(x) and φ 2(x) and suppose that their Fourier transforms $${\psi _1}(\xi ) = F{\phi _1}(x),{\psi _2}(\xi ) = F{\phi _2}(x)$$ (1.1) exist. The Fourier transform of the product φ 1(x) · φ 2(x) is $$F\{ {\phi _1}(x){\phi _2}(x)\} = {\text{ }}\int_{ - \infty }^\infty {{\phi _1}(x){\phi _2}(x){e ...
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