to trace, verify, or otherwise piece together Chen’s
 5   financial condition:
 6              Unexplained deposits and withdrawals:   Relying on the bank
 7   statements produced, Petteys declared that there were $2,329,000
 8   in unexplained deposits and $2,244,000 in unexplained
 9   withdrawals from Chen’s accounts for the years 2014 and 2015.
10              201st Court Property:   Relying on Chen’s testimony and the
11   documents produced, Petteys declared that she was unable to
12   verify the source of the funds used to purchase the 201st Court
13   Property.               -10-
 1   under 28 U.S.C. § 158.4
 2                                 III.   ISSUE
 3           Did the bankruptcy court err when it granted summary
 4   judgment and denied Chen’s discharge under § 727(a)(3)?
 5                          IV.   STANDARD OF REVIEW
 6


Saudi developer ACWA Power reached financial close for the development, construction and operation of three photovoltaic projects worth $190 million and set for peak total output of 165.5 megawatts at the Benban complex in Upper Egypt's Aswan, the company announced in a press release Monday.

Out of the $190 million, 75% will be financed through a non-recourse project debt from the European Bank for Reconstruction and Development and the Industrial and Commercial Bank of China.

The Multilateral Investment Guarantee Agency is covering the remaining 25% of the project’s cost which is financed with equity capital.

Construction of the three power plants will begin in Q1 2018 and the projects will be operational by Q4 2018.

“We are very excited that our first projects in Egypt have not only achieved financial close but
config.Formatters.JsonFormatter.SerializerSettings.PreserveReferencesHandling
     = Newtonsoft.Json.PreserveReferencesHandling.Objects;

How can I configure Azure Function Json Serializer, to allow it?

A:

Looking at the overloaded methods, I found:

then I used it with this code:
var serializerSettings = new Newtonsoft.Json.JsonSerializerSettings()
{
    ReferenceLoopHandling = Newtonsoft.Json.ReferenceLoopHandling.Serialize,
    PreserveReferencesHandling = Newtonsoft.Json.PreserveReferencesHandling.All
};

return new JsonResult(p, serializerSettings);

And it worked.
{
  "$id": "1",
  "Parent": null,
  "Name": "TONY",
  "Children": {
    "$id": "2",
    "$values": [
      {
        "$id": "3",
        "Parent": {
          "$ref": "1"
        },
        "Name":


24.6% (3.4 trillion KRW), the costs for loss of productivity by healthcare utilization were 13.0% (1.8 trillion KRW), and the costs for loss of productivity by premature death were 62.4% (8.6 trillion KRW). In this study, the socioeconomic cost of injuries in Korea between 2001 and 2003 was estimated by using not only health insurance claims data, but also automobile insurance, IACI claims and mortality data. We conclude that social efforts are required to reduce the socioeconomic cost of injuries in Korea, which represented approximately 1.9% of the GDP for the time period specified.Hopefully, I’ll make some new running buddies!

Find the next state for me and my mom to cross off. While we’ve been focusing on training for Bay State recently, it’s not going to get us closer to our 50 state goal. Life was a little hectic this summer with me starting a new job, but things are finally settling down again, and it’s time for us to start planning. Pennsylvania, New Jersey, and Delaware are all possibilities that would be a little closer to home, but it’s going to be trickier to find races up in this area as the weather gets colder.

Incorporate more interval/tempo runs into my workouts. I started doing this this summer since I was so intent on my 5k PR, and I actually really like


, after six years of planting, 700,000 mangroves are growing; providing stock feed for sheep and habitat for oysters, crabs, other bivalves, and fish.

Seventy percent of mangrove forests have been lost in Java, Indonesia. Mangroves formerly protected the island's coastal land from flooding and erosion. Wetlands International, an NGC based in the Netherlands, in collaboration with nine villages in Demak where lands and homes had been flooded, began reviving mangrove forests in Java. Wetlands International introduced the idea of developing tropical versions of techniques traditionally used by the Dutch to catch sediment in North Sea coastal salt marshes. Originally, the villagers constructed a sea barrier by hammering two rows of vertical bamboo poles into the seabed and filling the gaps with brushwood held in place with netting. Laterin diabetic rats. In an oral glucose tolerance test, treatment with Z. officinale was found to decrease significantly the area under the curve of glucose and to increase the area under the curve of insulin in STZ-diabetic rats. Treatment with Z. officinale also caused a decrease in serum cholesterol, serum triglyceride and blood pressure in diabetic rats. Our data suggest a potential antidiabetic activity of the juice of Z. officinale in type I diabetic rats, possibly involving 5-HT receptors.


combination of natural binding, target sequence and expression in response to different stresses across studies, we would have the opportunity to address a variety of important p53 universe issues at the mechanistic as well as the network level and to identify genes that are directly targeted by p53 for altered expression.

The advent of genome-wide chromatin immunoprecipitation of DNA fragments followed by high-throughput sequencing (ChIP-seq) coupled with gene expression provides a potential means to addressing the above issues. In the last seven years, multiple studies have been published, often with differences in results potentially due to biological variation, technical issues, or method of analysis. Here, we examined 44 data sets from human p53 ChIP-seq studies that contained activated or overexpressed p53 binding and associated gene expression. We also analyzed25th--75th percentile, black line = median, and whiskers = 1.5 \* interquartile range (IQR). Open symbols are outliers for each genomic region. (**B**) Distribution of called peaks on chromosome 5 in some normal (GM00011, GM6170, HFK) and cancer (MCF-7, U2OS) cells after DXR or Nutlin-3 treatment. Data set reference citations are in () following the peak descriptions.](gky720fig1){#F1}

We addressed the distribution of p53 binding across chromosomes. As shown in [Supplementary Figure SF4](#sup1){ref-type="supplementary-material"}, peaks are distributed across the genome in a non-random manner, which may simply reflect the non-randomness of genome structure. All chromosomes show a clustering of peaks in several chromosomal regions, and the clustering was similar for all cell types examined. Importantly, as shown in the example for Chromosome 5 (Figure [1B](#F1){ref-type="fig"}), peak regions were distributed similarly in


shown. The inset summarizes the distribution of p53 motifs for the 943 cistrome targets and for the 2375 genes, with a p53 motif containing peak in ≥2 data sets near the TSS, that had no change in expression. (**C**) Overlap of p53 cistrome genes with previously identified p53 targets. (**D**) IPA signaling pathways of the 713 potential new p53 cistrome target genes (with a Fisher\'s Exact test *P*-value \< 1 × 10^−3^).](gky720fig3){#F3}

We also examined whether p53 cistrome genes were more likely to contain a perfect p53 consensus motif. Even though 54 perfect motifs located near a TSS were frequently bound across data sets, only 25 are associated with changes in expression, corresponding to 24 cistrome genes (the perfect motif with one spacer has a similar ratio (11/22)) ([Supplementarysimilar ChIP-seq signal as peaks with a motif may not be surprising. Analysis of how p53 is bound at commonly bound sites should be possible using current mass spectrometry techniques to determine the bases and amino acid residues crosslinked.

p53 binding and transcription {#SEC4-2}
-----------------------------

Many questions about p53 and its transcriptional network are addressable through our meta-analysis and p53 BAER hub. For example, we investigated the influence of p53 motif and non-motif binding sites on expression as well as the potential effect of other p53 targets (such as lncRNAs and miRNAs) on gene expression, whether p53 is a direct transcriptional repressor, as well as the significance of the extensive p53 whole genome binding revealed by multiple ChIP-seq studies that, so far, has not been associated with changes in gene expression.

In


same criteria (see Materials and Methods), the DEGs in each study represent potential valid p53 regulated genes regardless of the number of studies in which they appear.

Among the cistrome genes, 659 (70%) are upregulated, 256 (27%) are downregulated and 28 can be either upregulated or downregulated. Downregulation has been proposed to be through an indirect mechanism. Recently, directly bound p53 was proposed to function only as an activator ([@B88],[@B89]). Repression by activated p53 was suggested to occur through the DREAM repression complex (DP, RB-like, E2F4, and MuvB) in a manner that requires p21 induction ([@B90]) or through the miRNA-mediated pathway ([@B65]) rather than by direct binding of p53 to motif targets. Of the p53 transcriptome genes in ≥2 data sets in our study, 533 (15%) correspond to DREAMnone of the 256 repressed cistrome genes appeared in more than three studies, 122 upregulated p53 cistrome genes were found in four or more studies. Furthermore, 3% of the p53 cistrome targets were found to be activated in some experimental conditions while repressed in others, suggesting repression may be cell or treatment specific. Contrary to what has been proposed, from our analysis we cannot exclude that p53 mediates direct gene repression at sites with or without the p53 motif. Repression could also be due, for example, to recruitment of co-repressors, or by displacement of specific activators from promoters due to the presence of overlapping binding sites.

The p53 cistrome is likely modulated by the nature and duration of the stress signal, the cell type, other TFs and cofactors, chromatin,


provided for vertically pivotal movement thereon so as to accommodate upward and downward movement between the towing vehicle and the vehicle towed. The closed end of the "A" shaped tongue portion of course mounts the trailer hitch coupler, which receives the corresponding ball component mounted to the tow vehicle. When not in use, the assembly must either be unbolted and removed from the vehicle before driving, or the tongue portion pivoted upwardly and locked into position with the hitch coupler projecting well above the hood of the car forwardly of the bumper thereof.
Since no side movement or telescoping movement is provided in these typical tow bars, hooking up of the vehicle can be tedious, as precise lateral and distal positioning of the tow car relative to the front& QCA_DDR_CFG_TRAS_MASK)       |\
	((_trcd  << QCA_DDR_CFG_TRCD_SHIFT)       & QCA_DDR_CFG_TRCD_MASK)       |\
	((_trp   << QCA_DDR_CFG_TRP_SHIFT)        & QCA_DDR_CFG_TRP_MASK)        |\
	((_trrd  << QCA_DDR_CFG_TRRD_SHIFT)       & QCA_DDR_CFG_TRRD_MASK)       |\
	((_trfc  << QCA_DDR_CFG_TRFC_SHIFT)       & QCA_DDR_CFG_TRFC_MASK)       |\
	((_tmrd  << QCA_DDR_CFG_TMRD_SHIFT)       & QCA_DDR_CFG_TMRD_MASK)       |\
	((_cas   << QCA_DDR_CFG_CAS_3LSB_SHIFT)   & QCA_DDR_CFG_CAS_3LSB_MASK)   |\
	((_opage << QCA_DDR_CFG_PAGE_CLOSE_SHIFT) & QCA_DDR_CFG_PAGE_CLOSE_MASK) |\
	(((_cas & 0x8) >> 3) << QCA_DDR_CFG_CAS_MSB_SHIFT)

/* DDR_CONFIG2 */
#define _qca_ddr_cfg2_reg_val(_burst_type, \


Piganna

Species

First Appearance

It is a mix between a pig and an iguana, has purple skin and a row of big dark purple spikes on its back. The mouth is the biggest part of the body and is full of razor-sharp teeth. It has only 2 fingers on each hand and foot.

It doesn't appear to have any kind of nose or nostrils at all: it could be argued that this is because the second species is not Iguana but rather Piranha, and it would have gills instead of a nose, but no visible gills are present on the creature either.The PM and Sonia Gandhi must walk on the streets without security.No they would not dare. They use the tax payers money to protect themselves and reel out pious platitudes and assurances which means nothing. The people are fed up with this lip service. Shameless to say that one percent cannot be prevented-what if that one percent is directed to the netas.Remember when Indira Gandhi was assassinated Rajiv Gandhi had the sinfulness and shamelessness to say that when the big tree falls the small plants around die. This he said to justify the genocide of the Sikhs. This is the kind of netas we have. Lives of people have no value.Does the value of a life depend on the background on the muscle and money power that person


authority and institutions because they/these have led down the people-have betrayed the people’s faith and trust. It must be remembered that AUTHORITY is not the criterion of TRUTH..It is the simple folks-the hardworking class, the starving millions of this country who still believe in national patriotism that have morphed into Baba Ramdev and Anna Hazare to demand the right to righteousness, to plead for a clean governance and for accountability to the people. It would be too simplistic for the GOI under the Congress to think that this movement can be crushed. That force can be used under constitutionality as it did in the Ramlila grounds to crush the rights of the people. State terrorism cannot be constitutional-the sovereignty of Parliament flows from the people and if theg - 2085311, -33*b - 5*g - 695085 = -34*b. Is b a composite number?
True
Let y(j) = -343*j + 28. Let a(x) = -86*x + 13. Let l(t) = -86*t + 14. Let f(u) = 7*a(u) - 6*l(u). Let c(p) = -9*f(p) + 2*y(p). Is c(8) prime?
False
Suppose -h = 3, 5*w - 2*h + 0*h = 6006. Let s = w - 5761. Is (-2)/8 + 1 + s/(-4) composite?
True
Suppose 0 = -3*t + 11 + 49. Let d be 10/(-25) + 6568/t. Suppose 0 = -m + 5*m - d. Is m a prime number?
False
Let w(p) = p. Let k(m) = -2927*m**2 - 12*m + 2. Let t(c) = -3*k(c) - 30*w(c). Is t(1) prime?
False
Let y(q) = -q**3 + 5*q**2 - 4*q - 3. Let l be


a prime number?
False
Let v(r) = 14*r**2 - 75*r - 889. Is v(-38) a composite number?
True
Let c = -788 + 793. Suppose c*o = 7265 + 50900. Is o a prime number?
True
Let f = -3 - -1. Let v(m) be the first derivative of 92*m**3/3 - m**2/2 - 5*m - 252. Is v(f) a prime number?
False
Let h be (-3)/2*-4*-6. Let d be 1388*(2 - h/(-21))*7. Let m = -1657 + d. Is m a composite number?
True
Is (-1)/(2 + 2) + 18374229/68 a prime number?
True
Let n(u) = 99813*u - 530. Is n(3) prime?
False
Let a(f) = f**2 - f + 1. Let n(m) = 51*m**2 - 2*m + 1. Let w(p) = -a(p) + n(p). Suppose 28*b - 71 = 13. Is w(b) composite?
True
Let y(o) = o. Let m(g) = -138*gFor Lisa Asvestas, owning a “local” business is a privilege and an opportunity.

“I think these kinds of businesses build community,” she said. “We need more of that.”

Asvestas owns 5 Points Local, a restaurant, yoga studio, and soon-to-be food market that officially opened its doors Tuesday morning. She and her staff served up coffee, juice, and breakfast tacos among other locally sourced, organic food items to a small group of community members and friends just northwest of downtown.

Anne Wolfe-Andersen, one of the managing partners at 5 Points, said the soft opening allowed the business to make a gradual introduction to the neighborhood.

“For the first day, we wanted people to know we were open, but we were also wanting to make sure we got the logistics down and make sure


just really feel a connection with this area, what it was in the past and what it can be,” she said. “I feel like the universe is moving us in this path and it’s the history of this area that is ready to blossom and really show itself.”

*Top image: The 5 Point Local kitchen is open for the public to see, adding to the local and clean feel. Photo by Kathryn Boyd-Batstone.

Related Stories:

Historic Southtown Firehouse to Become Italian Restaurant

O’liva Keeps San Antonio Local at Plaza de Armas

Lake/Flato Architects Celebrate 30 Years of Local, International Work

Hemisfair Seeks Local Businesses to Fill Historic Homesforces Vincent to lie to his colleagues, cheat his partner, steal a duffel bag filled with cocaine, and weave his way through the labyrinthine nightclub that serves as headquarters for a sneering kingpin. Most of the movie takes place in and around this overcrowded hot spot, with Vincent being chased or impeded by his cowardly partner, an overeager rookie cop, an intense internal affairs officer, a psychotic triggerman, and two batches of drug dealers thirsting for a fight. Often movies set in one location feel static and confined, but Sleepless Night never loses its edge, finding new inspiration in each room of this gargantuan club. Fight scenes break out on dance floors, in bathroom stalls and even the kitchen—where in a frenzied attempt to get the upper hand


language is verified with a program written with the system design language.
In the process of designing circuitry, it often happens that a program developed with the general-purposed programming language differs from a circuit (i.e., a program) written with the system design language. This is because the circuit design involves an error. If two resultant programs do not match, a cause of it is needed to be traced in the circuit.
To find an error, a function such as “printf” is often used to indicate a value of an internal variant A. The function “printf” is referred to as a character string output function in the C-language. This function “printf” is added into the program of the general-purposed programming language, and the program is executed. Also, in the program written---
abstract: 'In the first part of this article I present a system of retarded coordinates based at an arbitrary world line of an arbitrary curved spacetime. The retarded-time coordinate labels forward light cones that are centered on the world line, the radial coordinate is an affine parameter on the null generators of these light cones, and the angular coordinates are constant on each of these generators. The spacetime metric in the retarded coordinates is displayed as an expansion in powers of the radial coordinate and expressed in terms of the world line’s acceleration vector and the spacetime’s Riemann tensor evaluated at the world line. The formalism is illustrated in two examples, the first involving a comoving world line of a spatially-flat cosmology, the other featuring an observer in


matching is carried out in Sec. III D, where we see that it does indeed produce Eq. (\[1.1\]).

This concludes the summary of the results contained in this paper. Various technical details are relegated to Appendices A and B. Throughout the paper I work in geometrized units ($G=c=1$) and with the conventions of Misner, Thorne, and Wheeler [@MTW:73]. Other applications of the retarded coordinates (including the fields produced by point particles, and their motion in curved spacetime) are featured in a recent review article [@poisson:03].

Retarded coordinates
====================

Geometrical elements
--------------------

To construct the retarded coordinates we must first introduce some geometrical elements on the world line $\gamma$ at which the coordinates are based. The world line is described by relations $z^\mu(\tau)$ with $\tau$ denoting proper time, its normalized tangent vector is $u^\mu = dz^\mu/d\tau$, andits acceleration vector is $a^\mu = D u^\mu/d\tau$ with $D/d\tau$ denoting covariant differentiation along the world line. Throughout we use Greek indices $\mu$, $\nu$, $\lambda$, $\rho$, etc. to refer to tensor fields defined, or evaluated, on the world line.

We install on $\gamma$ an orthonormal tetrad that consists of the tangent vector $u^\mu$ and three spatial vectors ${e^{\mu}_{a}}$. These are transported on the world line according to $$\frac{D {e^{\mu}_{a}}}{d \tau} = a_a u^{\mu}
+ \omega_a^{\ b} {e^{\mu}_{b}},
\label{2.1.1}$$ where $a_a(\tau) = a_{\mu} {e^{\mu}_{a}}$ are the frame components of the acceleration vector and $\omega_{ab}(\tau) = -\omega_{ba}(\tau)$ is a prescribed rotation tensor. Setting $\omega_{ab} = 0$ would make the triad Fermi-Walker transported on the world line, and in many applications this would be a sensible choice. We nevertheless allow the spatial


angles $\theta^A$. A canonical choice for the parameterization is $\Omega^a = (\sin\theta \cos\phi, \sin\theta \sin\phi,
\cos\theta)$. It is then convenient to perform a coordinate transformation from $\hat{x}^a$ to $(r,\theta^A)$, using the relations $\hat{x}^a = r \Omega^a(\theta^A)$. (Recall from Sec. II C that the angles $\theta^A$ are constant on the generators of the null cones $u
= \mbox{constant}$, and that $r$ is an affine parameter on these generators. The relations $\hat{x}^a = r \Omega^a$ therefore describe the behavior of the generators.) The differential form of the coordinate transformation is $$d\hat{x}^a = \Omega^a\, dr + r \Omega^a_A\, d\theta^A,
\label{2.7.1}$$ where the transformation matrix $$\Omega^a_A \equiv \frac{\partial \Omega^a}{\partial \theta^A}
\label{2.7.2}$$ satisfies the identity $\Omega_a \Omega^a_A = 0$.

We introduce the quantities $$\Omega_{AB} = \delta_{ab} \Omega^a_A \Omega^b_B,
\label{2.7.3}$$ which act as a (nonphysical) metric in the subspaceR_{0a} \Omega^a + R_{ab} \Omega^a \Omega^b \bigr) + O(r^3) \Bigr],
\label{2.7.16}$$ where $\Omega$ is the determinant of $\Omega_{AB}$; in the canonical parameterization, $\sqrt{\Omega} = \sin\theta$.

Specialization to $a^\mu = 0 = R_{\mu\nu}$
------------------------------------------

In this subsection we specialize our previous results to a situation where $\gamma$ is a geodesic on which the Ricci tensor vanishes. We therefore set $a^\mu = 0 = R_{\mu\nu}$ everywhere on $\gamma$, and for simplicity we also set $\omega_{ab}$ to zero.

It is known that when the Ricci tensor vanishes, the Riemann tensor can be decomposed in terms of a timelike vector $u^\alpha$ and two symmetric-tracefree, spatial tensors ${\cal E}_{\alpha\beta}$ and ${\cal B}_{\alpha\beta}$ (see, for example, Ref. [@thorne-hartle:85]). In terms of frame components we have $$\begin{aligned}
R_{a0b0}(u) &=& {\cal E}_{ab}
\nonumber \\
R_{a0bc}(u) &=& \varepsilon_{bcd} {\cal B}^d_{\ a},
\label{2.8.1} \\
R_{acbd}(u)


In these expressions the dependence on retarded time $u$ is contained in ${\cal E}_{ab}$ and ${\cal B}_{ab}$, while the angular dependence is encoded in the unit vector $\Omega^a$.

It is convenient to introduce the irreducible quantities $$\begin{aligned}
{\cal E}^* &=& {\cal E}_{ab} \Omega^a \Omega^b,
\label{2.8.5} \\
{\cal E}^*_a &=& \bigl(\delta_a^{\ b} - \Omega_a \Omega^b \bigr)
{\cal E}_{bc} \Omega^c,
\label{2.8.6} \\
{\cal E}^*_{ab} &=& 2 {\cal E}_{ab}
- 2\Omega_a {\cal E}_{bc} \Omega^c
- 2\Omega_b {\cal E}_{ac} \Omega^c
\nonumber \\ & & \mbox{}
+ (\delta_{ab} + \Omega_a \Omega_b) {\cal E}^*,
\label{2.8.7} \\
{\cal B}^*_a &=& \varepsilon_{abc} \Omega^b {\cal B}^c_{\ d} \Omega^d,
\label{2.8.8} \\
{\cal B}^*_{ab} &=& 2\bigl(\delta_{(a}^{\ e}
- \Omega_{(a}\Omega^e \bigr) \varepsilon_{b)cd}
\Omega^c {\cal B}^d_{\ e}.
\label{2.8.9}\end{aligned}$$ These are all orthogonal to $\Omega^a$: ${\cal E}^*_a \Omega^a =
{\cal B}^*_a \Omega^a =0$ and ${\cal E}^*_{ab} \Omega^b =
{\cal B}^*_{ab} \Omega^b = 0$. In terms of these Eqs. (\[2.8.2\])–(\[2.8.4\]) become $$\begin{aligned}
S_{ab} &=& {\cal E}_{ab}^* + \Omega_a {\cal E}^*_b + {\cal E}^*_a
\Omega_b + \Omega_a \Omega_b {\cal E}^*
\nonumber \\ & & \mbox{}
+ {\cal B}^*_{ab} + \Omega_a {\cal B}^*_b + {\cal B}^*_a \Omega_b,
\label{2.8.10} \\
S_{a} &=& {\cal E}^*_a + \Omega_a {\cal E}^* + {\cal B}^*_a,
\label{2.8.11} \\
S &=& {\cal E}^*.
\label{2.8.12}\end{aligned}$$

When Eqs. (\[2.8.10\])–(\[2.8.12\]) are substituted into the metric tensor of Eqs. (\[2.6.3\])–(\[2.6.5\]) — in which $a_a$ and $\omega_{ab}$ are both set equal to zero — we obtain the compact expressions $$\begin{aligned}
g_{uu} &=& - 1 - r^2 {\cal E}^* + O(r^3),
\label{2.8.13} \\
g_{ua} &=& -\Omega_a + \frac{2}{3} r^2 \bigl( {\cal E}^*_a
+ {\cal B}^*_a \bigr) + O(r^3),
\label{2.8.14} \\
g_{ab} &=&


d\theta^A d\theta^B = d\theta^2 +
\sin^2\theta\, d\phi^2$. While $\bar{u}$ is a retarded-time coordinate and $\rho$ is a radial coordinate, these are distinct from $u$ and $r$, and Eq. (\[2.9.5\]) does not match the form of Eq. (\[2.9.4\]). Since $u$ and $\bar{u}$ can both be used to label light cones centered at $\rho = 0$, there must exist between them a relation of the form $u = u(\bar{u})$. And since $r$ and $\rho$ can both be used to parameterize the null generators of a light cone $\bar{u} = \mbox{constant}$ (although $\rho$ is not an affine parameter), there must exist between them a relation of the form $r=r(\bar{u},\rho)$. We shall now obtain these relations. We recall that the world line is located at $\rho = r = 0$.

In the coordinates $(\bar{u},\rho,\theta,\phi)$, the observer’swork in a neighborhood of $\rho=0$, and $a^2(\bar{u}+\rho)$ can be expressed as a Taylor expansion. This yields $$r = a \rho \biggl[ 1 + \frac{a'}{a} \rho + \frac{1}{3}
  \biggl( \frac{a''}{a} + \frac{a^{\prime 2}}{a^2} \biggr) \rho^2
+ O(\rho^3) \biggr],$$ where a prime indicates differentiation with respect to $\bar{u}$; here and below, the scale factor and its derivatives are evaluated at $\rho=0$ and expressed as functions of $\bar{u}$ only. From this we gather that $r_{\bar{u}} = a' \rho + a''
\rho^2 + O(\rho^3)$, and Eq. (\[2.9.10\]) gives $$g_{uu} = -1 + \biggl( \frac{a''}{a}
- \frac{a^{\prime 2}}{a^2} \biggr) \rho^2 + O(\rho^3)$$ and $$g_{AB} = a^2 \rho^2 \Omega_{AB} \biggl[
1 + 2 \frac{a'}{a} \rho + \biggl( \frac{a''}{a}
+ \frac{a^{\prime 2}}{a^2} \biggr)\rho^2 + O(\rho)^3 \biggr].$$ Expressing these results in terms of $r$ instead of


calculated in Sec. III C by linearizing the field equations about the metric of the background spacetime.

The metric ${\sf g}(\mbox{external zone})$ is a functional of a world line $\gamma$ that represents the motion of the small black hole in the background spacetime. Our goal is to obtain a description of this world line, in the form of equations of motion to be satisfied by the black hole; these equations will be formulated in the background spacetime. It is important to understand that fundamentally, $\gamma$ exists only as an external-zone construct: It is only in the external zone that the black hole can be thought of as moving on a world line; in the internal zone the black hole is revealed as an extended object and the notion of a${\sf g}(\mbox{external zone})$ is a functional of a world line $\gamma$ while ${\sf g}(\mbox{internal zone})$ contains no such information, [*matching the metrics necessarily determines the motion of the small black hole in the background spacetime*]{}.

Matching the metrics of Eqs. (\[3.1.1\]) and (\[3.1.2\]) in the buffer zone can be carried out in practice only after performing a transformation from the external coordinates used to express ${\sf g}(\mbox{external zone})$ to the internal coordinates employed for ${\sf g}(\mbox{internal zone})$. The details of this coordinate transformation are presented in Appendix C and the end result of matching is revealed in Sec. III D.

Metric in the internal zone
---------------------------

To proceed with the program outlined in the previous subsection we first calculate the internal-zone metric and replace Eq. (\[3.1.1\]) by a more concrete expression. We recall that the


\bar{r}^2 \bar{{\cal E}}^*
+ O(\bar{r}^3/{\cal R}^3), \\
{\sf g}_{\bar{u}\bar{r}} &=& - 1, \\
{\sf g}_{\bar{u}\bar{A}} &\to&
\frac{2}{3} \bar{r}^3 \bigl( \bar{{\cal E}}^*_A
+ \bar{{\cal B}}^*_A \bigr) + O(\bar{r}^4/{\cal R}^3), \\
{\sf g}_{\bar{A}\bar{B}} &\to& \bar{r}^2 \bar{\Omega}_{AB}
- \frac{1}{3} \bar{r}^4 \bigl( \bar{{\cal E}}^*_{AB}
+ \bar{{\cal B}}^*_{AB} \bigr) + O(\bar{r}^5/{\cal R}^3),    \end{aligned}$$ where $$\begin{aligned}
\bar{{\cal E}}^* &=& {\cal E}_{ab} \bar{\Omega}^a \bar{\Omega}^b, \\
\bar{{\cal E}}^*_A &=& {\cal E}_{ab} \bar{\Omega}^a_A \bar{\Omega}^b, \\
\bar{{\cal E}}^*_{AB} &=& 2 {\cal E}_{ab} \bar{\Omega}^a_A
\bar{\Omega}^b_B + \bar{{\cal E}}^* \bar{\Omega}_{AB}  \end{aligned}$$ and $$\begin{aligned}
\bar{{\cal B}}^*_A &=& \varepsilon_{abc} \bar{\Omega}^a_A
\bar{\Omega}^b {\cal B}^c_{\ d} \bar{\Omega}^d, \\
\bar{{\cal B}}^*_{AB} &=& 2 \varepsilon_{acd} \bar{\Omega}^c
{\cal B}^d_{\ b} \bar{\Omega}^{(a}_A \bar{\Omega}^{b)}_B  \end{aligned}$$ are the tidal gravitational fields that were first introduced in Sec. II H. Recall that $\bar{\Omega}^aV_{\alpha\beta\mu\nu}(x,z) u^\mu u^\nu\,
d\tau
\nonumber \\ & & \mbox{}
+ 4 m \int_{-\infty}^{\tau_<}
G_{\alpha\beta\mu\nu}(x,z) u^\mu u^\nu\, d\tau
\nonumber \\
&\equiv& 4 m \int_{-\infty}^{u^-}
G_{\alpha\beta\mu\nu}(x,z) u^\mu u^\nu\, d\tau
\label{3.3.12}\end{aligned}$$ is the “tail part” of the gravitational potentials. Notice that I have introduced a short-hand notation in the last line of Eq. (\[3.3.12\]); the important point is that the integral of $G_{\alpha\beta\mu\nu}(x,z) u^\mu u^\nu$ up to $\tau = u^-$ avoids the singular behavior of the Green’s function on the light cone $\sigma(x,z) = 0$.

We must next express Eq. (\[3.3.11\]) in the form of an expansion in powers of $r/{\cal R}$. For this we shall need the expansion [^4] $$U_{\alpha\beta\gamma'\delta'} u^{\gamma'} u^{\delta'} =
g^{\alpha'}_{\ (\alpha} g^{\beta'}_{\ \beta)} \Bigl[ u_{\alpha'}
u_{\beta'} + O(r^3/{\cal R}^3) \Bigr],$$ which contains no terms at order $r/{\cal R}$ or $(r/{\cal


h^{\rm tail}_{0ac} \Omega^c \bigr)
+ \bigl( h^{\rm tail}_{ab0} + h^{\rm tail}_{abc} \Omega^c \bigr)
\biggr]
\nonumber \\ & & \mbox{}
+ O(mr^2/{\cal R}^3).
\label{3.3.26}  \end{aligned}$$

Matching: motion of the black hole in the background spacetime
--------------------------------------------------------------

Comparison of Eqs. (\[3.2.9\])–(\[3.2.11\]) and Eqs. (\[3.3.24\])–(\[3.3.26\]) reveals that the internal-zone and external-zone metrics do no match in the buffer zone. But as the metrics are expressed in different coordinate systems, this mismatch is hardly surprising. A meaningful comparison of the two metrics must therefore come after a transformation from the external coordinates $(u,r\Omega^a)$ to the internal coordinates $(\bar{u},\bar{r}\bar{\Omega}^a)$. This transformation is worked out in Appendix C, and it puts the external-zone metric in its final form $$\begin{aligned}
{\sf g}_{\bar{u}\bar{u}} &=& - 1 - \bar{r}^2 \bar{\cal E}^*
+ O(\bar{r}^3/{\cal R}^3)
\nonumber \\ & & \mbox{}
+ \frac{2m}{\bar{r}} + \bar{r} \biggl[\Omega^{\prime a}
+ h^{\rm tail}_{ab}(u') \Omega^{\prime a} \Omega^{\prime b}
\Bigr], \\
x''_a &=& x'_a
+ \frac{1}{2} h^{\rm tail}_{ab}(u') x^{\prime b},  \end{aligned}$$ and it affects the metric at orders $m/{\cal R}$ and $mr/{\cal R}^2$. After performing this transformation the metric becomes $$\begin{aligned}
{\sf g}_{u''u''} &=& -1
- r^{\prime\prime 2} {\cal E}^{\prime\prime *}
+ O(r^{\prime\prime 3}/{\cal R}^3)
\nonumber \\ & & \mbox{}
+ \frac{2m}{r''} + r'' \biggl[ 4m {\cal E}^{\prime\prime *}
- 2 \biggl(a_a -\frac{1}{2} h^{\rm tail}_{00a} + h^{\rm tail}_{0a0}
\biggr) \Omega^{\prime\prime a} \biggr]
+ O(mr^{\prime\prime 2}/{\cal R}^3), \\
{\sf g}_{u''a''} &=& -\Omega''_a
+ \frac{2}{3} r^{\prime\prime 2} \bigl(
{\cal E}^{\prime\prime *}_a  + {\cal B}^{\prime\prime *}_a \bigr)
+ O(r^{\prime\prime 3}/{\cal R}^3)
\nonumber \\ & & \mbox{}
+ r'' \biggl[ - \frac{4m}{3}
\bigl( {\cal E}^{\prime\prime *}_a + {\cal B}^{\prime\prime


<?xml version="1.0" encoding="UTF-8"?>
<Workspace
   version = "1.0">
   <FileRef
      location = "group:KBKit.xcodeproj">
   </FileRef>
   <FileRef
      location = "group:Pods/Pods.xcodeproj">
   </FileRef>
</Workspace>
comments.

"The ideological content of these movements is somewhat different from country to country, obviously. They're both generally anti-Muslim, and they're both generally anti-tax."

Obviously Tea Partiers are anti-tax, though most would probably say they are anti-spending, but what's the evidence they are anti-Muslim? And, while we're at it, what's the evidence to link O'Keefe with the Tea Party? I'd say the author mistakenly conflates the "far right," Conservatives, Republicans and the Tea Party.


A few months ago I came across a photograph of the Andromeda galaxy (M31) that completely took my breath away. It was simply beautiful. When I discovered it was taken by a 16 year old, I could not believe it and I was simultaneously green with envy and extremely awestruck. Jacob Bers was the photographer and I remember contacting him not long after he published his M31 photograph asking for his permission to use the image in one of my older blog posts. Later, I contacted Jacob again and asked him if I could print and frame his photograph for my dining room. He gave permission and I wanted to share with you this beautiful image and its place in my home. The photograph below shows M31 inphotograph that I have captured is tie between my recent M31, and my M42 I took at Yosemite last year. My M42 was the first serious attempt at deep-sky astrophtography I made, and thinking back on it, I am very surprised it worked. I took it on Christmas Eve at a view point in Yosemite. I had never tested the lens I was using, nor had I really tested the mount. I had no guiding, and no telescope. All I was using was a lens and a camera on my new equatorial mount. I was only able to get 2 min exposures (I can now get up to 20 min exposures) and I had no idea what to expect from them. I got home from Yosemite thinking that


your earliest astronomy memory or the first thing you remember looking at through a telescope?

JB: I remember when I was about 5 I looked through a small scope at the moon. I thought it was cool, but Thomas the Tank Engine was on, and as a 5 year old, nothing beats Thomas. Now that I’m an astrophotographer, however, I’ve learned to loathe the moon’s blinding presence in our sky.

JL: What is your next AP challenge or objective?

JB: My next AP challenge is going to likely be a deep picture of the Horsehead nebula. The Horsehead nebula is one of the more challenging objects in the sky for DSLR astrophotographers due to the fact that most of its light comes in the form of Hydrogen Alpha light. Hydrogen alphaQ:

Opening image files with Sentinel 2 toolbox

Anyone worked with the Sentinel-2 toolbox/SNAP? It doesn't support sentine-2 data to be opened directly. I tried opening  .safe, .zip and .xml files.

A:

After unzipping, you should find an xml file inside the root directory with the same name as the zipped file. Select the xml file and be patient because opening the file takes a little while. You can then view the data per band, or right click on the scene name to open an RGB composite.

Normally this should also work directly from the zip file.
However, you should note that the zip files are sometimes corrupted during the download, which seems to be te case with your file. In other words, I think that you are doing the


in captivity and often subjected to repeated rape by multiple men, while others were taken as militants’ “wives” and forced to cook, clean, and collect food or water.

Most victims said they had not received post-rape medical or mental health care such as drugs to prevent HIV and unwanted pregnancy, citing a lack of health facilities, the cost of services or transport, and misconceptions about available services.

Thirteen women out of the 296 survivors interviewed said they had been children at the time of the attacks and become pregnant as a result of the rapes, according to the HRW.

“During attacks, fighters whipped women and girls, tied them up for long periods, burned them, and threatened them with death,” the HRW report said, adding that survivors reported injuries ranging from brokenfears the referendum, which 175,000 people are eligible to vote in, could inflame tensions between indigenous Kanak people, who tend to favour independence, and the white population, which boiled over into deadly violence in the 1980s.

The quasi-civil war claimed more than 70 lives. It led to the 1998 Noumea Accord which paved the way for the steady devolution of powers as well as Sunday’s referendum.

On Friday, separatist activists drove along Noumea’s waterfront in a convoy of around 20 cars, waving the Kanak flag to cries of “Kanaky” – their name for New Caledonia.

Separatists have urged Kanak voters to choose self-determination, throwing off the shackles of “colonial” authorities in Paris. But indigenous people make up less than 50% of the electorate and some Kanaks back staying part of France,


the way ViewPager creates Fragments doesn't expose me to the FragmentTransaction.
class MyViewPagerAdapter extends FragmentStatePagerAdapter {
    public MyViewPagerAdapter(FragmentManager fm) {
        super(fm);
    }

    @Override
    public Fragment getItem(int i) {
        if (i == 0) {
            return MyFragment.newInstance();
        } else if (i == 1) {
            return MyFragment.newInstance();
        } else if (i == 2) {
            return MyFragment.newInstance();
   Q:

android: layout: How to make my dialog box fill the screen with the XML

I'm trying to get a Dialog box to open covering most the screen (by that I mean it still has its nice  rounded effect but cover the content behind)
I've been trying with fill parent but it keeps behaving like a wrap content
<?xml version="1.0" encoding="utf-8"?>
<LinearLayout xmlns:android="http://schemas.android.com/apk/res/android"
    android:layout_width="fill_parent"
    android:layout_height="fill_parent"
    android:orientation="vertical"
    android:layout_centerHorizontal="true"
 >

<LinearLayout
    android:gravity="center_horizontal"
    android:orientation="vertical"
    android:layout_width="fill_parent"
    android:layout_height="fill_parent">
    <SurfaceView android:id="@+id/surface"
        android:layout_width="400px"
        android:layout_height="200px"
        android:layout_centerHorizontal="true">
    </SurfaceView>


u / t_{\rm c}$\end{document}$, where *t*~c~ = β/Ω. We consider β in the range 7 ≤ β ≤ 25, to investigate the dependence of the collision velocity on the strength of the gravitational perturbation, while remaining safely in the range in which fragmentation does not occur in 2D (Young & Clarke [@bib72]) as well as minimizing the influence of artificial viscosity heating on the spiral structure.

4. DISC MODEL AND INITIAL CONDITIONS {#sec4}
====================================

For the gas disc model, we take a central mass *M*~⋆~ = 1 and disc mass *M*~D~ = 0.1. For the disc structure, we use an initial surface density profile Σ ∝ *R*^−2^, between *R*~in~ = 1 and *R*~out~ = 5, which ensures the same resolution in *h*/*H* everywhere. We set up the disc with an initial Toomre parameter*Q* = 2, and evolve it for 10^3^ inner dynamical times, approximately nine cooling times at the outer edge, allowing the self-gravitating structure to reach a steady state before introducing the dust.

The dust particles are given an initially uniform density with the same Σ ∝ *R*^−2^ density distribution as the gas. The simulations have then been run for a further 100 to 300 inner dynamical times, until the dust velocity distribution has stopped varying. For our canonical simulations, we use 10^6^ particles per phase. We use the same number of gas neighbours for both the gas and dust particles, *N*~NGB~ = 50, which corresponds to *h*/*H* ≈ 0.2. It is worth noting that our chosen kernel, the Wendland C^6^, is 1.35 times wider than the commonly used cubic spline kernel, such


dispersion is correctly reproduced. However, the correlation times at small separations are not. For this reason, our 'noisy' initial conditions, which remove the effects of the smallest scales and save computational time, are the best choice.

In Fig. [2](#fig2){ref-type="fig"}, we show the gas and dust surface density for St = 3 and 10, which provides a useful reference for interpretation of the collision velocities. The dust surface density scale is arbitrary due to the use of the test-particle limit; for reference we scale the density such that the unperturbed gas and dust surface density are equal. The range St = 3--10 bridges the region where the width of the dust spiral features is the same as those in the gas, with St = 3 showing dense spiral arms and regionsThe solid lines denote means for resolved/unresolved pairs and the black dashed lines are included as approximate bounding boxes for the *N* = 10^6^ case to guide the eye. Increasing the resolution causes resolved pairs to move to lower separations at the same velocity, while unresolved pairs move to both lower separations and lower velocities.](stw488fig4){#fig4}

When we present our results, we will (for each value of the Stokes number) present particle velocity dispersions considering only the resolved particles and also those including the unresolved too -- evidently the fraction of unresolved particles varies with both Stokes number and resolution (λ~sam~). The way that such plots (Fig. [7](#fig7){ref-type="fig"}) should be interpreted is that the resolved values represent a true representation of the velocity dispersion of that particle subset; in the cases


thick with opacity dominated by ice grains. The relevant radial scalings for such a disc are *c*~s~ ∝ *R*^−1.5^, ρ ∝ *R*^−3^ and ΔΣ/Σ ∝ β^−0.5^ ∝ *R*^9/4^. This regime extends inwards to the point where ice grains sublime (around 15 au for this accretion rate). A radius of 30 au corresponds to β = 150 which we estimate as being the inner limit for which trapping in spirals is effective, given grains of a suitable Stokes number. Fig. [17](#fig17){ref-type="fig"} illustrates the radial dependence of Stokes number and collision velocity as a function of particle size given our model disc (see the figure caption for details).

![Left: Stokes number as a function of radius for differing particle sizes adopting the analytic self-gravitating disc model of Clarke ([@bib10]). The black dashed line shows the boundary between the Epstein and Stokes dragfriction limit for smaller Stokes numbers. For St \> 1, the scaling of relative velocity with cooling time-scale (β) is taken from the results of Fig. [13](#fig13){ref-type="fig"}.](stw488fig17){#fig17}

Answering the question posed above then boils down to determining whether collision velocities are small enough to permit growth to St = 0.3 at radii \>30 au (noting that at such radii the grains are expected to be icy).[^7^](#fn7){ref-type="fn"} If we fold together the radial scalings given above and the expression for the differential radial drift of dust in multi-sized dust populations, we find that the differential drift velocity between two particles with fixed sizes scales as $$\documentclass[12pt]{minimal}
\usepackage{amsmath}
\usepackage{wasysym}
\usepackage{amsfonts}
\usepackage{amssymb}
\usepackage{amsbsy}
\usepackage{upgreek}
\usepackage{mathrsfs}
\setlength{\oddsidemargin}{-69pt}
\begin{document}
}{}\begin{equation*} \Delta v_{\rm drift} \propto R^{15/4}, \end{equation*}\end{document}$$with radius since it is associated with a fixed Stokes number and, for our assumed disc structure, St ∝ *R*^3^.


St = 1, this results in λ~stop~ \< *H* for *R* \< 60 au and thus driving by self-gravity *density* fluctuations will be inefficient, making equa-tion ([15](#equ15){ref-type="disp-formula"}) an overestimate of the velocity dispersion. Instead, we expect that the dominant driving of velocity *dispersion* at smaller radii and St ∼ 1 may be the turbulent gas velocity, which is also weaker at longer cooling times (Shi & Chiang [@bib60]). Therefore, we expect that the typical masses should be less than those estimated from equation ([15](#equ15){ref-type="disp-formula"}) (≈4.5 × 10^−5^(ρ~d~/ρ~g~)^−1/2^ M~⊕~ at 30 au), with 10 or 100 km planetesimals perhaps more typical outcomes than Moon-mass or Ceres-mass objects.

Finally, we note that even though we have shown that growth to St \> 0.3 (and hence significant particle concentration) requires *icy* grains, even silicate grains with conn2 = turn_port_->CreateConnection(udp_port_->Candidates()[0],
                                         Port::ORIGIN_MESSAGE);
    conn1->Ping(0);
    EXPECT_TRUE_SIMULATED_WAIT(conn2->receiving(), kSimulatedRtt, fake_clock_);
  }

  void TestTurnSendData(ProtocolType protocol_type) {
    PrepareTurnAndUdpPorts(protocol_type);

    // Create connections and send pings.
    Connection* conn1 = turn_port_->CreateConnection(udp_port_->Candidates()[0],


be set to SOCKET_ERROR.
  EXPECT_EQ(SOCKET_ERROR, turn_port_->error());
}

// Testing turn port will attempt to create TLS socket on address resolution
// failure.
TEST_F(TurnPortTest, TestTurnTlsOnAddressResolveFailure) {
  turn_server_.AddInternalSocket(kTurnTcpIntAddr, PROTO_TLS);
  CreateTurnPort(kTurnUsername, kTurnPassword,
                 ProtocolAddress(rtc::SocketAddress("www.google.invalid", 3478),
                                 PROTO_TLS));
  turn_port_->PrepareAddress();
  EXPECT_TRUE_WAIT(turn_error_, kResolverTimeout);
  EXPECT_EQ(SOCKET_ERROR, turn_port_->error());
}

// In case of UDP on address resolve failure, TurnPort will not create socket
// and return allocate failure.
TEST_F(TurnPortTest, TestTurnUdpOnAddressResolveFailure) {
  CreateTurnPort(kTurnUsername, kTurnPassword,
                 ProtocolAddress(rtc::SocketAddress("www.google.invalid", 3478),
 conspired to possess cocaine with intent to distribute is sufficient if, viewing the evidence in the light most favorable to the government, any rational trier of fact could have found the defendant guilty beyond a reasonable doubt of the elements of the crime.   United States v. Sharif, 817 F.2d 1375, 1377 (9th Cir.1987).

3
The evidence showed that on December 6, 1985, Daniel Serrano placed a package in the trunk of his BMW, and that he then drove to an El Toro parking lot and met Guzman next to a Toyota van.  After a brief conversation, the two men switched cars, with Guzman driving off in the BMW while Serrano followed in the van.  Guzman led Serrano to downtown Los Angeles, and the men parked some


---
abstract: 'We report the direct observation of the non-reciprocity of the velocity of light, induced in a gas by electric and magnetic fields. This bilinear magneto-electro-optical phenomenon appears in the presence of crossed electric and magnetic fields perpendicular to the light wavevector, as a refractive index difference between two counterpropagating directions. Using a high finesse ring cavity, we have measured this magneto-electric non-reciprocity in molecular Nitrogen at ambient temperature and atmospheric pressure; for light polarized parallel to the magnetic field it is $2\eta_{\parallel \;{\mathrm{exp}}}(\mathrm{N_2})= (4.7\pm 1)\times 10^{-23}\;\mbox{m.V}^{-1}\mbox{.T}^{-1}$ for $\lambda =1064\;$nm, in agreement with the expected order of magnitude. Our measurement opens the way to a deeper insight into light-matter interaction, since bilinear magneto-electric effects correspond to a coupling beyond the electric dipole approximation. We were able to measurenext step will be to use rotatable rods to measure MENR for different fields orientations. Applying parallel electric and magnetic fields will also allow us to measure magneto-electric Jones birefringence and check that it is indeed equal to $\eta_\perp + \eta_\parallel$, as it should be [@Graham1983_84; @Robilliard2011]. A vacuum tank presently under construction will allow us to improve our measurement precision and to study different gases, among which atomic gases such as Krypton and Xenon, where relativistic effects are expected to be significant. Our experiment demonstrates that many effects that were previously beyond experimental reach can now be measured in quite reasonable timescales. Our long term goal is to search for the magneto-electric non-reciprocity of quantum vacuum [@Rikken2003; @Robilliard2011], which is approximately $7\times 10^8$ times smaller than what


Q:

Copy text from template into mail (Lotus Notes)

I'm trying to create a toolbar button that inserts a footer (including some buttons) into the current mail.
As far as I know, theres no way to create and modify buttons directly with Lotus Formula, so I'm trying to copy/paste from another document. I can't use a mail template because I need the text to be inserted in replies.
This is what I have assembled from online examples:
@PostedCommand([FileOpenDatabase]; "SERVER" : "mailbox.nsf"  ;
    "($All)" ; "" ; 1 ; 1 ) ;
@PostedCommand([OpenDocument] ; "" ; "34884517EED80C33C125A999005301D4") ;
@PostedCommand([EditDocument]) ;
@PostedCommand([EditGotoField] ; "Body" ) ;
@PostedCommand([EditSelectAll]) ;
@PostedCommand([EditCopy]) ;
@PostedCommand([FileCloseWindow]) ;
@PostedCommand([FileCloseWindow]) ;
@PostedCommand([EditPaste])

This works inconsistently, depending on what I am looking at when pressing the button.
Sometimes it opens a search box with the actualtext of the mail pasted in it. It does seem to close the new mail.
I'm especially confused because many commands don't take any arguments, eg FileCloseWindow. How do I control the "context" of the commands or check for success?
It feels like doing automation with SendKeys - fire off a chain of commands and hope that nothing unexpected happens. Of course, I am a total noob with Lotus Formula, so I may be doing this totally wrong. Any help is appreciated.

A:

You may want to use Alan Lepofsky's free "Paste Information" application.
The Notes database "Paste Information" serves as the repository for the content you wish to reuse. Move the cursor to the position where you want to insert the text, click on the "Paste Information" Toolbar icon and then choose


[Théodore Simon (1873-1961). The career of a psychiatrist involved in the professionalization of psychiatric nurses].
Well-known for having created the famous Metric Scale of Intelligence along with the psychologist Alfred Binet (1857-1911), what is less known is that Théodore Simon (1873-1961) was also a major actor of the professionalization of psychiatric nurses in France. From his engaged textbook published in 1911 to his journal, explicitly titled ?L'Infirmier Psychiatrique,? which he created in 1953 via the specialized school he founded and directed between 1946 and 1957 at the Maison Blanche hospital in Neuilly-sur-Marne, Simon worked throughout his career for the acknowledgment and the training of those he considered as true partners. This is what we want to demonstrate in this paper, which redraws the forgotten career history of this militantto Satan as ‘satan,’ with a lower case ‘s.’ I’ve seen this sort of thing before, but I’ve never understood the logic. Sure, he might be the prince of darkness, but does that mean we have to throw out the basic rules of written English whenever his name comes up. And don’t get me started on K.D. Lang… 😉

Some of the flaws are far more serious and, to my thinking, render it useless (at best) to dangerous (at worst, but quite likely.) Allow me to share an example.

There is a section that treats the importance of the Bible in the Salvation Army. There are a couple of paragraphs that discuss 2 Timothy 3:16 and the high number of ancient manuscripts available. Then we get this, on page 16:

The


//
// basic_serial_port.hpp
// ~~~~~~~~~~~~~~~~~~~~~
//
// Copyright (c) 2003-2012 Christopher M. Kohlhoff (chris at kohlhoff dot com)
// Copyright (c) 2008 Rep Invariant Systems, Inc. (info@repinvariant.com)
//
// Distributed under the Boost Software License, Version 1.0. (See accompanying
// file LICENSE_1_0.txt or copy at http://www.boost.org/LICENSE_1_0.txt)
//

#ifndef BOOST_ASIO_BASIC_SERIAL_PORT_HPP
#define BOOST_ASIO_BASIC_SERIAL_PORT_HPP

#if defined(_MSC_VER) && (_MSC_VER >= 1200)
# pragma once
#endif // defined(_MSC_VER) && (_MSC_VER >= 1200)

#include <boost/asio/detail/config.hpp>

#if defined(BOOST_ASIO_HAS_SERIAL_PORT) \
  || defined(GENERATING_DOCUMENTATION)

#include <string>
#include <boost/asio/basic_io_object.hpp>
#include <boost/asio/detail/handler_type_requirements.hpp>
#include <boost/asio/detail/throw_error.hpp>
#include <boost/asio/error.hpp>
#include <boost/asio/serial_port_base.hpp>
#include <boost/asio/serial_port_service.hpp>

#include <boost/asio/detail/push_options.hpp>

namespace boost {
namespace asio {

/// Provides serial port functionality.
/**
 * The basic_serial_port class template provides functionality that is common
 * to all serial ports.
 *
 * @par Thread Safety
 * @e Distinct @e objects: Safe.@n
 * @e Shared @e objects: Unsafe.
 */
template <typename SerialPortService = serial_port_service>
class basic_serial_port
  : public basic_io_object<SerialPortService>,
    public serial_port_base
{
public:
  /// (Deprecated: Use native_handle_type.) The *
   * @param io_service The io_service object that the serial port will use to
   * dispatch handlers for any asynchronous operations performed on the port.
   *
   * @param device The platform-specific device name for this serial
   * port.
   */
  explicit basic_serial_port(boost::asio::io_service& io_service,
      const std::string& device)
    : basic_io_object<SerialPortService>(io_service)
  {
    boost::system::error_code ec;
    this->get_service().open(this->get_implementation(), device, ec);
    boost::asio::detail::throw_error(ec, "open");
  }

  /// Construct a basic_serial_port on an existing native serial port.
  /**
   * This constructor creates a serial port object to hold an existing native
   * serial port.
   *
   *


* This function may be used to obtain the underlying representation of the
   * serial port. This is intended to allow access to native serial port
   * functionality that is not otherwise provided.
   */
  native_type native()
  {
    return this->get_service().native_handle(this->get_implementation());
  }

  /// Get the native serial port representation.
  /**
   * This function may be used to obtain the underlying representation of the
   * serial port. This is intended to allow access to native serial port
   * functionality that is not otherwise provided.
   */
  native_handle_type native_handle()
  {
    return this->get_service().native_handle(this->get_implementation());
  }

  /// Cancel all asynchronous operations associated with the serial port.
  *
   * @param ec Set to indicate what error occurred, if any.
   */
  boost::system::error_code send_break(boost::system::error_code& ec)
  {
    return this->get_service().send_break(this->get_implementation(), ec);
  }

  /// Set an option on the serial port.
  /**
   * This function is used to set an option on the serial port.
   *
   * @param option The option value to be set on the serial port.
   *
   * @throws boost::system::system_error Thrown on failure.
   *
   * @sa SettableSerialPortOption @n
   * boost::asio::serial_port_base::baud_rate @n
   * boost::asio::serial_port_base::flow_control @n
   * boost::asio::serial_port_base::parity @n
   * boost::asio::serial_port_base::stop_bits @n
   * boost::asio::serial_port_base::character_size
   */
  template <typename SettableSerialPortOption>


 template <typename GettableSerialPortOption>
  boost::system::error_code get_option(GettableSerialPortOption& option,
      boost::system::error_code& ec)
  {
    return this->get_service().get_option(
        this->get_implementation(), option, ec);
  }

  /// Write some data to the serial port.
  /**
   * This function is used to write data to the serial port. The function call
   * will block until one or more bytes of the data has been written
   * successfully, or until an error occurs.
   *
   * @param buffers One or more data buffers to be written to the serial port.
   *
   * @returns The number of bytes written.
   *
   * @throws boost::system::system_error Thrownatherosclerotic heart disease (CAD), but the relationship between the development of AMI and γδ T cells is still not clear. In addition, the expression of γδ T cell subgroup populations in patients with AMI has not yet been reported. Based on previous literature and data, we hypothesized that γδ T cells play a key role in the pathogenesis and pathophysiology of AMI. The present study was designed to investigate the expression pattern and clonality of TCR repertoire of γδ T cells in AMI patients, analyze the expression levels of regulatory genes Forkhead box P3 (Foxp3) and Interleukin-17A (IL-17A), and characterize the correlation between γδ T cells and the pathogenesis of AMI.

Methods {#Sec2}
=======

Participants {#Sec3}
------------

25 patients (aged 64.4 ± 11.7 years, 17 males and 8 females) diagnosed with STEMI admitted to First Affiliated


patients, but that was highly expressed in healthy individuals. The high clonal expansion frequencies of the TCR Vδ8, TCR Vδ4 and TCR Vδ3 were determined in AMI patients. We suggested that such expanded TCR Vδ8, TCR Vδ4 and TCR Vδ3 T cell clones might be reactive T cell clones directed against AMI. It might have certain clinical significance in the screening and prediction of AMI. However, this hypothesis requires confirmation with a larger cohort.

It is known that the immune response of the body mainly includes cellular and humoral immunity, and the specific cellular immunity mediated by T cells is particularly important. Decades ago, it was found that another important function of T cells is immune suppression or immunologic tolerance. Tregs, a general term for a cell population ofAssociation of yeast RNA polymerase I with a nucleolar substructure active in rRNA synthesis and processing.

Abstract

A novel ribonucleoprotein complex enriched in nucleolar proteins was purified from yeast extracts and constituents were identified by mass spectrometry. When isolated from rapidly growing cells, the assembly contained ribonucleic acid (RNA) polymerase (pol) I, and some of its transcription factors like TATA-binding protein (TBP), Rrn3p, Rrn5p, Rrn7p, and Reb1p along with rRNA processing factors, like Nop1p, Cbf5p, Nhp2p, and Rrp5p. The small nucleolar RNAs (snoRNAs) U3, U14, and MRP were also found to be associated with the complex, which supports accurate transcription, termination, and pseudouridylation of rRNA. Formation of the complex did not depend on pol I, and the complex could efficiently recruit exogenous pol I into active ribosomal DNA (rDNA) transcription


“The academic world is a jungle,” wrote Schinner, who first applied statistical analytics to the manuscript more than a decade ago, “and like in any jungle, it is not recommended to show even potential weakness.”

Read: Has a mysterious medieval code really been solved?

All we know for certain, through forensic testing, is that the manuscript likely dates to the 15th century, when books were still mostly handmade and rare. But its provenance and meaning are uncertain, making it virtually impossible to corroborate any claims about its contents against other historical materials.

So why are so many scholars and scientists driven to solve the puzzle? For many, it’s the ultimate opportunity to prove their analytical skills in their given field. For others, it’s a chance to test promising new digital technologiesfailed to produce any evidence, through testimony or otherwise, that his confession was coerced; thus, we cannot find that the trial court erred in denying his motion to suppress his confession. This issue is without merit.

II. OVERWHELMING WEIGHT OF THE EVIDENCE
¶ 13. In his final issue on appeal, Sullivan argues that the verdict is against the overwhelming weight of the evidence. Sullivan contends that the State failed to admit competent evidence that proved he had committed the crime. "When reviewing a denial of a motion for a new trial based on an objection to the weight of the evidence, we will only disturb a verdict when it is so contrary to the overwhelming weight of the evidence that to allow it to stand would sanction an unconscionable injustice."


seal the sides of the opening as well as other various purposes. The drilling apparatus generally comprises a drawworks assembly which includes a cable drum, driving apparatus for rotatably driving the cable drum, a main brake and a secondary brake often referred to as a mode absorber. The drawworks performs various functions including raising and lowering the drilling pipe and bit for bit replacement, and connection of additional stands of drill pipe as well as to control drilling pressure. Also, the drawworks may be used to assist in installation of the casing as well as replacement thereof should the casing become worn due to extended drilling operations. The main brake is commonly intimately associated with the cable drum of the drawworks operating to stop and hold the drillingWho We Are

Students for Education Reform develops college students into grassroots organizers who fight for educational justice in their communities.

Our experiences and stories of overcoming educational inequality are undeniable and validate the demand for transformative change in our K-12 system. We fight for high academic standards, access to quality teachers and the right for families to choose the best school for their child, especially in communities that have historically been left behind.

What We Seek

One day, Americans will choose to offer universal quality public education. For the first time in our nation’s history, all students and communities will have access to a public education worthy of their dignity, talents, and limitless potential.

Educational justice cannot be achieved unless schools are safe, academically challenging, and inspire every child to reach their


limitless potential. We envision: A system of thriving accessible and quality schools that gives each child – regardless of race or socioeconomic background – the opportunity to succeed in college and in life. A school system where teachers and parents hold high expectations for students and work relentlessly to ensure no student falls through the cracks. A system where schools in which every family can choose a school and academic path that is right for their child.

SFER organizes college students to be a powerful force for K-12 education policy and political change through campus chapters that work at the national, state, and local levels to advocate for great teachers and quality school choices for all kids.

SFER primarily serves first-generation college students, students of color, and students from low-incomein the recent Supreme Court case, United States v. Jones, Justice Sotomayor said that she thought the Third Party Doctrine was outdated, while she and four other Justices -- including Justice Alito -- raised concerns about the information gathered by our

cellphones.

The Eighties Were Good for a Lot of Things -- But Not Sustainable Email Privacy Law

It's not just the Constitution, however. Congress has made clear that certain forms of data are protected by federal statute as well. Following the Katz decision, Congress passed the Wiretap Act in 1968, supplementing the strong Fourth Amendment privacy protections in phone conversations by enacting a comprehensive set of federal statutes. These statutes were designed to ensure that law enforcement has a compelling reason before intercepting phone calls.

And as electronic communication started to


e}_\omega$ with $\omega=\pm 1,0$: &&[**e**]{}\_[+1]{}=-

1\
i\
0

,\_0=

0\
0\
1

,\_[-1]{}=

1\
-i\
0

,\
&&|[**e**]{}\_[+1]{}=-(1,-i,0) ,|[**e**]{}\_0=(0,0,1) ,|[**e**]{}\_[-1]{}=(1,i,0) . Further, define f\^(P,)&=&(,  [**e**]{}\_+) ,\
|f\^(P,)&=&(,  |[**e**]{}\_+) . The Rarita-Schwinger wave functions are given by group-theoretical expressions corresponding to the addition of spins 1 and 1/2: \[eq:Rarita\] u\^(P,)&=&\_[,]{} 1 1/2|3/2f\^(P,)u(P,) ,\
|u\^(P,)&=&\_[,]{} 11/2|3/2 |u(P,)|f\^(P,) , with $\langle \ldots\rangle$ the appropriate Clebsch-Gordan coefficients. These wave functions obey the equations &&(P-E\_R)u\^(P,)=0 , P\_u\^(P,)=\_u\^(P,)=0 ,\
&&|u\^(P,)(P-E\_R)=0 ,|u\^(P,)P\_=|u\^(P,)\_=0 , and the identities \_u\^(P,)|u\^(P,) &=&-(g\^-\^\^-+) ,\
\_|u\^(P,) u\_(P,’)&=&-2E\_R\_[’]{} . Below, we shall restrict ourselves to the case of the $\Delta N\gamma^*$ transition. However, the formalism can be directly generalized to particles with any spin. The three-point function for this transition takes the form \[eq:doublepole\_NDg\] F\^(P,Q)&=&i\^2d\^4Xd\^4Ye\^[iPX-iQY]{}0|TO\^(X)J\^(0)|(Y)|0\
&=& \_[,]{} u\^(P,) P,|J\^(0)|Q, |u(Q,) + . Here, $O^\mu(X)$ and $\psi(Y)$ denote the $\Delta$ and nucleon interpolating field operators, respectively, $J^\rho$ is the electromagnetic current,\[eq:threepoint\] 0|[O]{}\_i(x\_0)J\^a(0)|Q,&=&U\_iX\_i\_[-]{}\^e\^[iP\_0x\_0]{} T(P\_0)\
&&(-iJ(P\_0)|F\_i\^[(A)]{}(p,|[**Q**]{}|)+F\_i\^[(B)]{}(p,|[**Q**]{}|)) . where $F_i^{(A)}(p,|{\bf Q}|)$ does not depend on $L$ (up to the exponentially suppressed contributions) and the indices $a,\varepsilon$ have been suppressed for brevity.

![Initial-state pion-nucleon interactions in the $\Delta N\gamma^*$ transition form factor. The quantity $\bar F_i$ denotes the sum of all irreducible diagrams.[]{data-label="fig:irreducible"}](irreducible1.eps){width="15.cm"}

The diagrams of the type (B) can be potentially dangerous. Indeed in the case of the elastic form factor, such diagrams lead to the so-called finite fixed points, see Ref.[@Hoja2]. However, the fact that one of the external particles (the nucleon) is stable simplifies matters considerably. As shown in section \[sec:analytic\] (see Eq. (\[eq:I1\])), in that case the quantity $\hat F_i^{(B)}(p,|{\bf Q}|))$ can be written as a product of two factors: F\_i\^[(B)]{}(p,|[**Q**]{}|))=-iJ(P\_0)|F\_i\^[(B)]{}(p,|[**Q**]{}|)) , \[eq:B\] where $\bar F_i^{(B)}(p,|{\bf Q}|))$, again, does not depend on $L$


the relativistic amplitude. Note that in the present paper we deal with the $P$-wave in the $\gamma^*p\rightarrow\pi^0p$ channel with the total isospin $I=3/2$ and total spin $J=3/2$. Below, we give the expressions, using the relativistic normalization of the Dirac spinors [@IZ].

The relativistic photoproduction amplitude can be written in the rest frame of the pion-nucleon system as \[eq:tmatrix\] T=8E \^(2)[F]{}(1), where $E$ is the total energy of the $\pi N$ system. The Pauli spinors $\chi(1)$, $\chi(2)$ carry the information on the spin states of the nucleons.

The matrix ${\cal F}$ has a decomposition (see, e.g., [@Drechsel]) \[eq:Drechsel\] [F]{} & = & iF\_[1]{} +()(())F\_[2]{} +i()()F\_[3]{} +i()()F\_[4]{}\
& & +i()()F\_[5]{} +i()()F\_[6]{}-\_0, where $\epsilon^\mu=(\epsilon_0,\,{\boldsymbol}\epsilon)$ is the photon polarization vector, $\hat {{\boldsymbol}k}={{\boldsymbol}k}/| {{\boldsymbol}k}| $ and $\hat {{\boldsymbol}q}={{\boldsymbol}q}/| {{\boldsymbol}q}| $ are the unit vectors for the photonstandards, health and safety possible, and demand will certainly grow as more nations electrify, and more vehicles are battery-powered.

Here are my fundamental assumptions: Wind turbines replace 100% of today’s 2.85 TW global electricity generation, by some future date – as many activists and politicians insist we must (and can) do. Turbines are all 1.8-MW nameplate power. Average turbine capacity factor gradually falls from 33% to 16.5% as the best wind sites are utilized, and much poorer sites must be developed.

(In the USA many of the best wind sites are off the Washington-to-California and Maine-to-Georgia coastlines, and in the Great Lakes, where water depths and powerful local opposition would make it impossible to install many turbines. Onshore turbine size is limited by the size of blades that can be


windless days, total power generation (and thus turbine numbers and land acreage) begins to skyrocket. For 48 hours of backup, triple the power generation; that’s the entire Lower 48. For a full week of backup, add in Canada.

Let’s not forget the transmission lines and batteries. They also need land (and raw materials).

How many batteries? Storing 1 gigawatt-hour (GWh) of electricity – to provide power for 48 windless hours for a US city of 700,000 people – would require 480,000 of Tesla’s new 100-kWh lithium-ion battery packs. Backing up 2.85 TW for just two windless days would require 1.4 trillion Tesla units! And this assumes the batteries are charged and discharged with 100% efficiency.

Just imagine the land, raw materials, mining, manufacturing and energy that would be needed to makeall those batteries (and replace them every few years). As energy and technology analyst Mark Mills has noted, all the world’s existing lithium battery factories combined manufacture only a tiny fraction of that.

I’m sure the world’s battery makers would be more than happy to take our hard-earned taxpayer and consumer cash to build more factories and make all those batteries – to save us from dangerous climate change that is no longer governed by the sun and other powerful natural forces.

Let’s get real. It’s time to stop playing with pixie dust and renewable energy utopia schemes. Time to open our schools and legislatures to actual thinking about energy, sustainability, climate change and what makes our jobs, health and living standards possible. Time for full-bore studies and legislative hearings


author of Eco-Imperialism: Green power – Black death and other books on the environment.

Note: My article fixing my previous math error has a stupid typo. It’s in the paragraph beginning “That clearly won’t work. The reference at the end of the paragraph to “1.8-GW turbines” should obviously read “1.8-MW turbines.”

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back seat forward
it's than comparable to other hatchbacks
like the volkswagen golf in the subaru
impreza I couldn't help but notice that
the anchors on the back roads which are
for securing child seats would easily
get in the way and maybe even damage
your car go because usually these things
are recessed overall I think bringing
the Astron was a good idea
the quality is good it's proven
technology and it has some upscale
features that you wouldn't get an entry
level compact car
for additional information on this car
or any other go to cars.com and our blog
kicking tires
[*et al.*]{}[@Birkedal] has a value in the range 0.19-0.22 for well widths between 80 and 160$\dot{A}$, while Kleinman predicts a value in the range 0.11-0.12. In order to explain this difference between theory and experiment, calculations were carried out with different techniques as well as with new assumptions[@different-ass] on the spatial form of the biexciton. Singh [*et al.*]{}[@different-ass] assumed a square-like arrangement of the electrons and the holes in a two dimensional biexciton which resulted in $f_H=0.228$. The latter approach is rather [*ad hoc*]{} and does not include the finite thickness of the biexciton and consequently is not able to explain the well width dependence of the biexciton binding energy.

The aim of the present paper is to explain the recent experimental results by considering localization effects on the


taken as a product of the 1D ground state wave functions for an electron (hole) in a hard wall quantum well. Averaging the Hamiltonian over the z-component ${\mathcal
  F}(z_{1e},z_{2e},z_{1h},z_{2h})=f_e(z_{1e})f_e(z_{2e})f_h
 (z_{1h})f_h(z_{2h})$ we obtain the following effective 2D Hamiltonian $$\begin{array}{rl}
\hat{H}_{\rho}=&\displaystyle\frac{1}{1+\sigma}(\sigma \Delta_a+\sigma
\Delta_b+\Delta_1 +\Delta_2 )-2(U_{1,a}+U_{1,b}+U_{2,a}+U_{2,b}-U_{a,b}-U_{1,2})
 \\ \\
  & \displaystyle +{1\over 4}
(1+\sigma) [ {1 \over \sigma} \omega^2
(\rho_a^2+\rho_b^2+\rho_1^2+\rho_2^2)],
\end{array}
 \label{secondham}$$ where $\sigma=m_e/m_h$ is the mass ratio between the electron and the hole and $U_{i,j}$ is the effective Coulomb potential obtained by averaging the real Coulomb potential over the wave functions along the z-direction. In Eq.(\[secondham\]) we expressed the energy in units of $R_y=e^2/2\epsilon a_B$ and the length in units of $a_B=\epsilon \hbar^2/e^2 \mu$ with $\epsilon$ the static dielectric constant and $\mu$ the in-plane reduced mass of the electron-hole system. Usingthat was caught laundering money as an example. In such cases, another middleman, like a government agency often steps in to handle the situation. But can we trust another centralized organization to solve a problem which was created by a centralized organization in the first place?

Sound Money

It is an excellent medium of exchange. While physical cash is still easier in many local situations, Bitcoin can be sent to all corners of the globe within a matter of minutes.

This inverse Bitcoin US Dollar chart gives us a big picture view of how cryptocurrencies are measuring up against paper. The Dollar has fallen dramatically since 2011:

This is not a mistake. The world’s reserve currency has lost 99.97% of its value against Bitcoin in this period. The trend is clear, people


all over the world are looking for a way to preserve their wealth.

Challenges

Of course, the cryptocurrency revolution comes with its own set of problems. A healthy level of skepticism is needed for any emerging technology. Scams, robbery and money laundering are still issues that affect the public at large. Scalability, large-scale adoption, and ease of use are some of the challenges developers face as they venture into uncharted territory.

Do We Really Need Cryptocurrencies?

Cryptocurrencies like Bitcoin are trying to solve some fundamental issues of the now 1000-year-old fiat based economy. We are in the early stages of this industry and there are probably more questions out there than answers.

Despite advances in technology, it is estimated that 1.7 billion people remain unbanked. How do we include them? Is there abetter way to facilitate global trade? Can we create sound community-based money? Do we really need cryptocurrencies? Well, when the next financial crisis hits, the ultimate question we may just have to ask ourselves is, can we really do without them?


of the levers of information remain firmly in progressives’ grip. Accordingly, it is difficult to avoid examining the resulting flow of information.

To be fair, America is a complex place. It would be an oversimplification to suggest there is a single version of the vision progressives have for America.

But it would not be a stretch to say that if a poll were taken among the elites of academia, the media, etc., they would name Ta-Nehisi Coates as one of our leading public intellectuals, perhaps topping the list. Coates tends to think about race in the same way as white nationalist Richard Spencer does, according to a convincing NYT op-ed.

Put another way, Coates tends to think about whites the way Jeong tweeted. The difference is that Coates is a much                               Plaintiff -   Appellee,

          versus

LESLIE FRANKLIN EVANS, III,

                                              Defendant - Appellant.

Appeal from the United States District Court for the Eastern
District of Virginia, at Norfolk. Raymond A. Jackson, District
Judge. (CR-95-192)

Submitted:   November 17, 2005


issue, the reduction in rpm's would not affect the wash process as drastically as you indicate.If the dishwasher is not filling properly, or if the detergent or rinse agent is "foaming" during the cycle, you will loose the pressure from the pump system and the top rack dishes will appear to not clean properly. Here's a quick easy check, start the dishwasher in any wash cycle, allow the unit to fill and wash for 3 to 5 minutes, unlatch the door,wait a few seconds, remove the lower rack. The water level in the bottom of the tub should cover the lower half of the heater element(at least) and the water temperature should be 120 dgrs.F. Allow the dishwasher to run a few more minutes and check for suds,the right side is black because the image I try to import in it has another type of array. The left image was an uint8 while the other is a "list". The second image is this one, which is saved from python:
enter image description here

A:

After a day of searching I found out that both variables can be changed to the type of a float64. The "list" variable:
Image = np.asarray(Image)

This creates an float 64 from a List variable. While the uint8 can be changed to a float64 by:
Image2=np.asarray(Image2/255)

Than the 2 can be combined with:
totalImgage = np.hstack((Image,Image2))

Which than creates the wanted image.


be obtained by changing the number (density) of holes concentrated to the side of the insulating layer 2 of the active layer 4.
Referring to the constitution illustrated in FIG. 1, the holes concentrated in the side of the insulating layer 2 are photo carriers generated by the irradiation of light. The density of the holes is determined by the wavelength and the quantity of light irradiated to the active layer 4. Thus, the resistance of the channel formed on the side of the gate insulating film 6 in the active layer 4 can be controlled by the light irradiated to the active layer 4.
It is confirmed by experimentation that a current change corresponding to about 104 to 105 times the photo carriers generated in the crystalline silicon activefor child in doc:
            if child.tag == 'Report':
                for item in child:
                    if item.tag == 'ReportHost':
                        print item.attrib

    except Exception as e:
        print e
        exit()
getDetails('file.nessus')

Example Output From Current Code
{'name': '172.121.26.80'}
{'name': '172.121.26.42'}
{'name': '172.121.26.41'}
{'name': '172.121.26.21'}
{'name': '172.121.26.15'}
{'name': '172.121.26.14'}

A:

Use item.get('name'). See https://docs.python.org/2/library/xml.etree.elementtree.html#xml.etree.ElementTree.Element.get for details.


try.

# "Firefox and Chrome use 300 ms"
# https://tools.ietf.org/html/rfc6555#section-6
# Though
#   https://www.researchgate.net/profile/Vaibhav_Bajpai3/publication/304568993_Measuring_the_Effects_of_Happy_Eyeballs/links/5773848e08ae6f328f6c284c/Measuring-the-Effects-of-Happy-Eyeballs.pdf
# claims that Firefox actually uses 0 ms, unless an about:config option is
# toggled and then it uses 250 ms.
DEFAULT_DELAY = 0.250

# How should we call getaddrinfo? In particular, should we use AI_ADDRCONFIG?
#
# The idea of AI_ADDRCONFIG is that it only returns addresses that might
# work. E.g., if getaddrinfo knows that you don't have any IPv6 connectivity,
# then it doesn't return any IPv6 addresses. And this is kinda nice, because
# it means maybe you can skip sending AAAA requests entirely. But in practice,
# it doesn't really work right.
#
# - on Linux/glibc, empirically, the default is to return all addresses, and
# with AI_ADDRCONFIG then it only returns IPv6 addresses if there is at least
# one non-loopback IPv6 address  they *don't* support multiple address bindings, like giving the ipv4 and
#   ipv6 addresses of the host.
#   I think maybe our semantics should be: we accept a list of bind addresses,
#   and we bind to the first one that is compatible with the
#   connection attempt we want to make, and if none are compatible then we
#   don't try to connect to that target.
#
# XX TODO: implement bind address support
#
# Actually, the best option is probably to be explicit: {AF_INET: "...",
#   AF_INET6: "..."}
# this might be simpler after
async def open_tcp_stream(
    host, port, *, happy_eyeballs_delay=DEFAULT_DELAY, local_address=None
):
    """Connect to the given host and port over TCP.

    If the given


being convinced of crimes against humanity by the Iraqi Special Tribunal.

19 Heinrich Himmler

Heinrich Himmler was the head of the SS, the second most powerful Nazi and the architect of the Final Solution. He, more than anyone, encouraged and facilitated Adolf Hitler’s decision to implement the Final Solution to the Jewish question, as well as other programs of ethnic cleansing that destroyed millions of lives during World War II. He was responsible for 6 to 7 million deaths of Poles, Russians, communists, and other groups whom the Nazis deemed unworthy to live including people with physical and mental disabilities. Himmler once said “The decision, therefore, lies here in the East; here must the Russian enemy, this people numbering two hundred million Russians, be killed on the battle field andwere others there for 6 years. They were blindfolded most of the time. They might have suffered a fate worse than death. He spread his ways across the Middle East. Saddam Hussein feared the spread of Khomeini’s militant brand of Shiism so he attacked Iran, which started the Iran-Iraq War, which caused the deaths of 1 to 2 million people. During the war, Khomeini sent young boys to fight and refused to make peace with Iraq even though there was at least one moment when Saddam offered peace for Iran. Because Khomeini refused to settle peace, Iran’s economy was ruined and 500,000 to 1 million Iranians were killed. His hatred of America and Western society inspired and paved the way for terrorist groups including Al-Qaeda. He paved the


to 90,000 Chinese. 100,000 civilians in the Philippines died from the Manila massacre. His men said that it was easy to kill because Hirohito told them that their lives were valueless compared to himself. He told his men to kill, burn, and loot all Chinese. Over 20 million Chinese, 10 million Asians in other countries, and millions of people in World War II were killed by the Japanese. He died in 1989 from cancer.

13 Nero

Nero was Rome’s 5th emperor from AD 54 to AD 68. He brought the Roman Empire to ruin. He burned entire cities. He murdered thousands of people including his aunt, stepsister, ex-wife, mother, wife and adoptive brother. He systematically murdered every member in his family. Some were killed in searing hot baths. He poisoned,a lions, panthers and bears and often killed gladiators. One gladiator alone was beaten up for 2 days full days. He sometimes ordered people to be killed by elephants. His cruelty caused people to commit suicide. He demanded sex with a lot of women including his 3 sisters. He would force husbands to give up their wives. He exiled his sisters and had his brother in law put to death. He caused many to die of starvation. Sawing people was one of his favorite things to do, which filleted the spine and spinal cord from crotch down to the chest. He liked to chew up the testicles of victims. He killed some of his most important friends and his father-in-law. One time Caligula said “I wish Rome had


IFN-gamma/lipopolysaccharide activation of macrophages is associated with protein kinase C-dependent down-modulation of the colony-stimulating factor-1 receptor.
IFN gamma/LPS treatment increases macrophage tumoricidal and microbicidal activity and inhibits CSF-1-induced macrophage proliferation. The mechanism underlying the latter effect was investigated in the CSF-1-dependent mouse macrophage cell line, BAC-1.2F5. IFN-gamma and LPS together dramatically reduced the total number of CSF-1 receptors (CSF-1R) via selective degradation of the cell surface form. Processing and transport of intracellular CSF-1R to the cell surface were unaffected. IFN-gamma alone had no effect but significantly enhanced LPS-induced CSF-1R down-regulation. The reduction in CSF-1R number was protein kinase C-dependent and involved changes in serine phosphorylation of the receptor at different sites. CSF-1R down-modulation by this mechanism may be important in switching off the energy-consuming processes of CSF-1R-mediated proliferation andessentially pocket the balance, which was estimated to be as high as 21% of the currency being recalled — or roughly $45 billion.

“Now it is not being explicitly stated — and in some cases they are going to deny it — but if a certain amount of cash does not come back then the central bank no longer has to account for that money,” said Arpan Nangia, the head of the India desk for HSBC’s commercial banking division. “So, for example, if a billion dollars does not come back then it's like a billion dollar profit for the central bank.”

Unfortunately for Modi and India’s central bank, this payday never materialized. As of now, over 82.5% of the recalled notes have been turned in, and it is estimated that


developing economies that also features Azerbaijan and Hungary at second and third positions, respectively. While India is placed at the 60th spot, many of the neighbouring nations are ahead in the rankings. China is ranked at the 15th position, Nepal (27th), Bangladesh (36th) and Pakistan (52nd).

The Inclusive Development Index (IDI) is based on 12 performance indicators. In order to provide a more complete measure of economic development than GDP growth alone, the index has three pillars — Growth and Development, Inclusion and Intergenerational Equity, and Sustainability.

This Is Just How Unequal is #India with top 1% Owning 58% of Wealth. #Modi #BJP http://blogs.wsj.com/indiarealtime/2017/01/17/this-is-just-how-unequal-india-is/ … via @WSJIndia

The richest 1% of Indians hold 58% of the country’s total wealth, according to Oxfam India.

The stark inequality in India is worse than thea higher share of total growth than the bottom 50% (12% vs. 11%), while the top 1% received a higher share of total growth than the middle 40% (29% vs. 23%).”

Last year, a report by Credit Suisse Research Institute said that the top 1% of the country’s population held 58.4% of its wealth, up from 53% in 2015. Within the BRICS group, only Russia’s wealthy controlled more of their country’s wealth. Since 2010, India has added a billionaire every 33 days and Indians’ share in the global billionaires’ club has grown from 1% to 5% over the last 20 years.Meanwhile, Piketty has also reiterated his demand for more transparency in sharing income tax data. Access to data is crucial in measuring inequality and understanding the distribution of wealth.


could probably have chosen another path," Dr Chancel told me.

Rising inequality is a global phenomenon. Oxfam’s briefings paper ‘An economy for the 99%’ reports only eight men today have the same wealth as 3.6 billion of the world’s population. In the last three decades seven out of 10 people living in a country have been facing inequality. Also the report mentions that in the next 25 years, the world will have its first trillionaire.

Besides this, every year economically stagnated countries cost $1,000 billion in the shape of corporate tax evasions. This huge sum can provide education to 124 million children and prevent the deaths of at least six million children globally. On the other hand, global inequality has devastating consequences for low-income countries like Pakistan.

The per capita incomeleast $20,000 a year, equates to roughly Hong Kong in terms of population and average income. The next 9% is akin to central Europe, in the middle of the global wealth pack. The next 40% of India’s population neatly mirrors its combined South Asian poor neighbours, Bangladesh and Pakistan. The remaining half-billion or so are on a par with the most destitute bits of Africa. To be sure, global companies take the markets of central Europe seriously. Plenty of fortunes have been made there. But they are no China.

Worse, the chances of India developing a middle class to match the Middle Kingdom’s are being throttled by growing inequality. The top 1% of earners pocketed nearly a third of all the extra income generated by economic growth between 1980


Only 3% of Indians have ever been on an aeroplane; only one in 45 owns a car or lorry. If nearly 300m Indians count as “middle class”, as HSBC has proclaimed, some of them make around $3 a day.

India's Richest 1% Cornered 73% Of Wealth Generated Last Year: Oxfam SurveyBesides, 67 crore Indians comprising the population's poorest half saw their wealth rise by just 1 per cent, as per the survey released by the international rights group Oxfam.

Besides, 67 crore Indians comprising the population's poorest half saw their wealth rise by just 1 per cent, as per the survey released by the international rights group Oxfam hours before the start of the annual congregation of the rich and powerful from across the world in this resort town.

The situationand education.

#Pakistan has the highest intergenerational income #mobility and the lowest #inequality among emerging economies. #WEF2018 #Davos https://www.weforum.org/agenda/2018/01/economist-plan-to-heal-fractured-societies/ …

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I am the Founder and President of PakAlumni Worldwide, a global social network for Pakistanis, South Asians and their friends. I also served as Chairman of the NEDians Convention 2007. In addition to being a South Asia watcher, an investor, business consultant and avid follower of the world financial markets, I have more than 25 years experience in the hi-tech industry. I have been on the faculties of Rutgers University and NED Engineering University and cofounded two high-tech startups, Cautella, Inc. and DynArray Corp and managed multi-million dollar P&Ls. I am a pioneer of the PC and mobile businesses and I have held senior management positions in


The Vampire Diaries' Damon and Elena: Find Out What Happens After Tonight's Big [Spoiler]!

Spoiler Alert: If you haven't watched last night's episode of The Vampire Diaries then get off the Internet stat! The following article contains lots of spoilers, so run away if you haven't fired up your DVR yet!
What's that sound? Oh, nothing. Just Damon (Ian Somerhalder) and Elena (Nina Dobrev) fans around the world having a collective coronary.
Allow us to join you: Gaaaaaaah!
Don't read another word if you haven't yet seen tonight's episode of The Vampire Diaries, but Damon and Elena finally did the horizontal mambo. Alas, this is The Vampire Diaries, a show that has basically redefined the term plot twist, so there's no happily ever after on the horizon...
The
»

IMDb.com, Inc. takes no responsibility for<?php

/**
 * @file Contains classes for data processing.
 *
 * Data processors can be used to process element arguments on evaluation time,
 * e.g. to apply input evaluators or to apply simple calculations to number
 * arguments.
 */

/**
 * Common base class for Rules data processors.
 */
abstract class RulesDataProcessor {

  /**
   * The processors' setting value.
   */
  protected $setting = NULL;

  /**
   * Allows chaining processors. If set, the next processor to invoke.
   */
  protected $processor = NULL;

  /**
   * Constructor.
   */
  protected function __construct($setting, $param_info, $var_info = array(), $processor = NULL) {
    $this->setting = $setting;
    $this->processor = $processor;
  }

  /**


as we need a
    // late binding to invoke the input evaluators version, if needed.
    $return = array();
    foreach ($this->processors() as $name => $info) {
      if (isset($processors[$info['class']])) {
        $return[$name] = $processors[$info['class']];
      }
    }
    return $return;
  }

  /**
   * Gets the settings of this processor.
   */
  public function getSetting() {
    return $this->setting;
  }

  /**
   * Processes the value. If $this->processor is set, invoke this processor
   * first so chaining multiple processors is working.
   *
   * @param $value
have announced they will remain closed through the 2019--2020 school year.Lift and enhanced tracing (LET) scenario: The "stay at home" order is lifted as in the previous scenario. Once partial reopening is implemented, we assume that 50% of symptomatic COVID-19 cases can be tested for SARS-CoV-2 infection, on average, within 2 days after the onset of symptoms and that they are isolated at home and their household members are quarantined successfully for 2 weeks (a sensitivity analysis for lower rate of isolation and quarantine is presented in the SM). We also assume that a fraction of the non-household contacts (we show results for 20% and 40%) of the symptomatic infections can be traced and quarantined along with their household as well - note that we consider that the


a large surge in the number of contact tracers. We have investigated what fraction of the population would be isolated/quarantined under the proposed contact tracing and isolation strategy. [Figure 4a](#F4){ref-type="fig"} shows the fraction of households that needs to be quarantined. Assuming the identification of 50% of the symptomatic infections, and tracing of 40% of their contacts and households, only about 9% of the population would be quarantined at any time. While this is certainly a relevant fraction of the population, it is a much better option if compared with massive social distancing policies affecting the entire population that last for months.

In [Table 1](#T1){ref-type="table"}, we report the number of symptomatic infections for which the contact tracing investigation should be performed in the basic scenarios. This number provides an estimateof the contact tracers per 1,000 individuals. It is important to note that the more effective is the contact tracing starting from each individual, the smaller is the number of generally traced households because the epidemic has lower incidence rates. In addition, as illustrated in [Figure 4b](#F4){ref-type="fig"}, the health status of the vast majority of quarantined individuals is unknown as contact tracing does not imply testing. The curves in [Figure 4a](#F4){ref-type="fig"} constitute the upper bounds for each simulated case. If we assume that the capacity to do massive testing would likely ramp up in the near future, then it is expected that the actual number of people in quarantine could be significantly lowered by testing the household. This would also alleviate the burden on household members that could


not go to work and increase compliance of isolation for the positive cases. It is also worth remarking that many of the logistic challenges faced with massive contact tracing might possibly be eased by digital technologies that are currently being investigated across the world following the examples of COVID-19 response in Asian countries^[@R23]^. Also it may be difficult to quarantine the entire household of individuals who are potentially exposed, since this is a hardship suffered with great uncertainty about their risk of infection. Offering other logistic quarantine solutions (quarantine centers, hotel rooms) might significantly raise the rate of compliance.

These results were obtained under several assumptions. There are very large uncertainties around the transmission of SARS-CoV-2, in particular, the fraction of sub-clinical and asymptomatic cases and their transmission. Estimatesof age-specific severity are informed from the analysis on individual-level data from China and other countries, and subject to change as more US data become available. We also do not include specific co-morbidities or pre-existing conditions of the specific BMA population. For this reason, in the [SM](#SD1){ref-type="supplementary-material"} we perform an extensive sensitivity analysis showing that the modeling results discussed here are robust to the plausible range of parameter values for the key time-to-event intervals of COVID-19 (e.g., incubation period, serial interval, and time from symptom onset to hospital admission, etc.). We are also not considering potential changes to the virus transmissibility due to environmental factors, in particular, seasonal drivers such as temperature and humidity. The modeling does not consider possible reintroduction of SARS-CoV-2 in the population from infected


of General Medical Sciences during the conduct of the study; AV reports grants and personal fees from Metabiota, Inc., outside of the submitted work; MC and APyP report grants from Metabiota, Inc., outside of the submitted work. The authors declare no other relationships or activities that could appear to have influenced the submitted work.

![Model components.\
Panel **a** is a schematic illustration of the weighted multilayer synthetic population built from mobility data in the metropolitan area of Boston. The agent-based system is made up by around 64000 adults and 21000 children, whose geographical distributions are shown in panel **b**. Nodes are connected by more than 5 million weighted edges. Community layers (that include workplaces), are further classified into categories according to Foursquare's taxonomy of places. Panel **c** displays the compartmentalquarantining their household and the households of a fraction of their contacts, as indicated in the legend of the bottom panels. Note that the vertical scales of panels **a, d**, and **g** are not the same and that both the number of new cases and total cases are per 1,000 inhabitants. In all panels the solid line represents the average over 10,000 simulations and the shaded region the 95% C.I.](nihpp-2020.05.06.20092841-f0002){#F2}

![Impact on the Boston health care system.\
Estimated number of individuals per 1,000 inhabitants that would need hospitalization (H), and intensive care (ICU) for each of the three scenarios considered in [Figure 2](#F2){ref-type="fig"}. Panel **a** corresponds to the unmitigated situation, whereas results for the LIFT and LET strategies are shown in panels **b** and **c**, respectively. The horizontal dotted-dashed lines