Q:

Diagnostic tools not working (VS 2015 Update 2 RTM)

I have an issue:
So I'm trying to profile my UWP / Metro (Win8.1) Apps. And keep facing the very same problem, - Diagnostic tools just won't work (Memory Usage specifically).
I keep getting errors like this:
"Failed to enable stack collection on heap trace session (0x8007007f)."
CPU usage turns on, but then it says: "Microsoft Visual Studio was unable to create a diagnostics report."
Would anyone explain me why is this happening and what are the possible workarounds?
Thank you in advance for your time spent to provide me with the solution!
P.S. I've been suffering from for ages and failed to find out how to tackle this :)

A:

Installing Update 2 RTM for Visual Studio 2015 helped me out!

would generate roughly $26 billion more in oil and gas revenues between 1980 and 1985enough to build four new oil sands plants. Under the existing tax and royalty regime, the provinces’share of the

industry’s $9.2-billion operating income last year was 46 per cent (or $4.3 billion). The corporations, largely foreignowned, took 44 per cent ($4.1 billion) while the federal bite was only 9.5 per cent ($876 million). Fully 30 per cent of Alberta’s share goes into the Heritage

Fund, an overstuffed savings account which, by next March, will stand at a staggering $6.2 billion. A $4 increase in price between 1980 and 1985 could create a kind of Saudi Alberta, with additional provincial revenues of $25 billion.

King Peter, understandably, has big plans for using the revenues from fastdepleting oil reserves


and his stumbling energy minister, Ray Hnatyshyn, were not convincing as they fled from a meeting with Lougheed and his energy minister, Merv Leitch, in a dingy, cinder-block motel in Saskatoon. Most experts, including federal officials, doubt that Ottawa can raise the same amounts from a profits tax—certainly not as readily—if only because companies are past masters at reducing their income through generous federal and provincial exploration incentives and depletion allowances. Some, such as Shell, don’t pay any tax at all. At week’s end, Crosbie seemed closer to candor when he admitted that without a tax of the kind favored by Ottawa, Clark’s goal of self-sufficiency by 1990 may have to be scrapped.

With the crisis in Iran entering its second chilling week, Clark did manage

to rally support onagain. On Monday, when Joe Clark hosted lunch for the premiers at 24 Sussex Drive, along with the porc Charcutière he served a modest Ontario vintage which, with two changes in spelling, was an unnecessary reminder of Ontario’s former petro glory. The label was Inniskillin Seyval Blanc. For Davis, the only consolation is that it costs $1,041.60 per barrel,

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INTRODUCTION
============

Friedreich's ataxia (FRDA) is an inherited degenerative disease that is characterized by progressive ataxia, including uncoordinated gait and limb movements, weakened muscle strength, and diminished senses of position and vibration. FRDA is caused by an insufficient level of Frataxin (FXN) ([@B1],[@B2]). FXN is an evolutionarily conserved mitochondrial protein that is involved in iron homeostasis in cells ([@B3])*.* Reduced levels of the *FXN* gene expression in FRDA patients are caused by a hyperexpanded tract of repeated GAA triplets in intron 1 of the *FXN* gene ([@B4],[@B5]). In FRDA patients, the GAA tract frequently consists of \>1000 triplets, whereas unaffected individuals have 66 or fewer repeats at the *FXN* gene ([@B4]). Pathological expansion of the GAA repeats is associated with localized chromatin changes and transcriptional silencing at the gene; however,and GFP\_(GAA·TTC)~560~\] were generated by integration of a tract of GAA repeats derived from the GM16210 affected cells as described previously ([@B9]). A DNA fragment harboring approximately 560 GAA repeats was PCR amplified from genomic DNA isolated from the GM16210 cell line (NIGMS Human Genetic Cell Repository at The Coriell Institute for Medical Research, Camden, NJ, USA) as described in ([@B9]). PCR product was cleaved by Bsu36I and BssHII endonucleases and the GAA repeat-containing fragment was cloned into intron 1 (1.2 kb from the exon1/intron1 junction) of the *GFP* gene of the pGFP_Int plasmid ([@B13],[@B14]). Plasmids containing 0 and 560 GAA repeats were integrated by site-specific recombination into the genome of the HEK293Flp-InT-Rex cell line (Invitrogen). The use of identical sites of integration for both GFP\_(GAA·TTC)~0~ and GFP\_(GAA·TTC)~560~ constructs


A agarose (Millipore) pre-blocked with BSA and salmon sperm DNA. The equivalent of 5 × 10^6^ (1 × 10^7^ cells in the case of RNA pol II ChIP) cells was immunoprecipitated overnight with 5 μg of antibodies recognizing histones and histone modifications (15 μg of RNA pol II antibody in the case of RNA pol II ChIP). The immunoprecipitates were immobilized on the pre-blocked protein A agarose beads for 1 h. Subsequently, the beads were washed with buffers containing low salt, high salt, and LiCl. Chromatin was eluted from the beads with elution buffer (100 mM NaHCO~3~ and 1% SDS) at room temperature for 15 min twice and subsequently subjected to the reverse cross-linking reaction using 5 M NaCl at 65°C for at least 5 h. The DNAs from chromatin complexes were isolated with Tris--EDTA buffer (80 mM Tris--HCl at1.Decreased level of *FXN* pre-mRNA downstream of the hyperexpanded GAA repeats. (**A**) Schematic diagram of the *FXN* gene. Black lines under the schematic diagram indicate regions amplified by designated primers used in this study. (**B**) *FXN* mRNA was analyzed in three control and three FRDA cell lines by qRT--PCR with primers complementary to the exons 3 and 4. Blue-series bars designate control cell lines, while Red-series bars designate FRDA cell lines. *FXN* expression was normalized to the expression level determined by control GM15851 cells. The experiment was conducted in triplicate. All data are expressed as mean ± SD. (**C**) Relative level of the *FXN* pre-mRNA was determined in various regions of the transcript. 'Up' and 'Down' primers amplify regions in the immediate vicinity of the GAA repeats. In1Ex2 and In2Ex3


cell lines. Importantly, levels of RNA pol II were not changed in the *FXN* promoter region (from −242 to −12) in FRDA cell lines compared to control cell lines, suggesting that *FXN* promoter activity is not affected in FRDA cell lines. These results are in agreement with previous findings that similar levels of *FXN* pre-mRNA at the region upstream of the GAA repeats are observed in both FRDA and unaffected control cell lines ([Figure 1](#F1){ref-type="fig"}C). Figure 2.Distribution of RNA polymerase II is affected in the region upstream of GAA repeats in FRDA cells. Level of total RNA pol II was determined by immunoprecipitating the large subunit of RNA pol II in FRDA and control cells. Average occupancy of RNA pol II across the *FXN* gene in all three*FXN* gene in FRDA cell lines. Similar to the mutated *FXN* gene in FRDA cells, introduction of the longer GAA repeats into a reporter gene results in formation of heterochromatin-like conformation and silencing of the transgene. The changes in the chromatin conformation triggered by the hyperexpanded GAA repeats are independent of transcription, indicating that the hyperexpanded GAA repeat tract is the primary inducer of the heterochromatin-like structures that subsequently inhibit the transcription process.

Comparison of histone modifications and RNA pol II distribution at the *FXN* gene between control and FRDA cell lines provides a strong indication that *FXN* deficiency in FRDA cell lines originates at a post-initiation step of transcription. Several reports using genome-wide approaches have suggested that post-initiation events are rate-limiting in the regulation of transcription ([@B19],[@B37]). This


*/

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1, -10deg);
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0);
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@keyframes bounceOutDown {
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  to {
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}

.bounceOutDown {
  -webkit-animation-name: bounceOutDown;
  animation-name: bounceOutDown;
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@-webkit-keyframes bounceOutLeft {
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-webkit-transform: none;
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.fadeInLeftBig {
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@-webkit-keyframes fadeInRight {
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  to {
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@keyframes fadeInRight {
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.fadeInRight {
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@-webkit-keyframes fadeInRightBig {
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0;
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@keyframes fadeOutLeft {
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  to {
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.fadeOutLeft {
  -webkit-animation-name: fadeOutLeft;
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}

@-webkit-keyframes fadeOutLeftBig {
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  to {
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    -webkit-transform: translate3d(-2000px, 0, 0);
    transform: translate3d(-2000px, 0, 0);
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}

@keyframes fadeOutLeftBig {
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  to {
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    -webkit-transform: translate3d(-2000px, 0, 0);
    transform: translate3d(-2000px,1;
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  to {
    -webkit-transform-origin: center;
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    -webkit-transform: rotate3d(0, 0, 1, 200deg);
    transform: rotate3d(0, 0, 1, 200deg);
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ease-in-out;
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@-webkit-keyframes zoomInUp {
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.slideOutRight {
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@-webkit-keyframes slideOutUp {
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@keyframes slideOutUp {
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  to {
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}

.slideOutUp {
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}

@keyframes cloudScroll {
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  to {


-webkit-transform: translate3d(-90%,0,0);
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}

@keyframes uncheck {
  0% {
    transform: translateX(26px);
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    transform: translateX(13px) scaleX(1.5);
  }
  40% {
    transform: translateX(0px) scaleX(0.75);
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  100% {
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}

@-webkit-keyframes uncheck {
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  100% {
    -webkit-transform: translateX(0px);
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@-moz-keyframes uncheck {
  0% {
    -moz-transform:perform Actions/Proxy Requests for attacker from Victim's browsers.

How Is It Exploited

Image link/ any link in email, on any website or on any blog .

CSRF can be done using Cross Site Scripting.

Malicious website can perform action using your authentication.

1. Image Link/Any Link In Email Or In Any Website

Server authenticates user and response from the server includes authentication cookie.

Without logging out, user visited a malicious website. That malicious website may contain malicious image link, post action to site user is logged in, malicious script or Ajax call which will be totally hidden from visitor. This is the "cross site" part of CSRF attack.

User will click the image or any button (filling forms and clicking submit), then browser will happily send the authentication cookie for the request because post request is


like (www.examplewebsite.com/account/delete) .

Request will run on server with the user's authentication and can perform any action, user is allowed to do.

This attack is tough to catch, and becomes worse when attacker does the post from AJAX. The victim will even not have to perform any action. This attack can breach even SSL because malicious user can send HTTPS request too like "https://examplewebsite.com/account/delete" .

2. XSS Can Also Be Used To do CSRF Attack

To learn XSS and prevention from it, please see my last article of this series.

POSTS/PUT/DELETE can also be forged. To prevent those, make requests unique and non-repeatable.

For ASP.NET Web Forms

ViewStateUserKey = Session.SessionID then viewstate will act as a form token

Protect SessionID using Hashing and Encryption

Use SSL to prevent sniffing of SessionID and ViewState

Either create a BasePage andb.
-4
Let n = 19 - 14. Suppose -5*r - n*m + 7 + 13 = 0, m - 20 = -5*r. Suppose -r*v + 5 = -7. Solve -o + v = -0*o for o.
3
Let v be ((-4)/10 + 2)/((-142)/(-355)). Solve 31 = -v*i + 23 for i.
-2
Suppose n - 27 = -2*t - 20, 24 = -4*t. Solve -5*x - n + 24 = 0 for x.
1
Suppose 329 - 30 = 44*s - 185. Solve 50 = s*r + 17 for r.
3
Suppose 36*a = 2*k + 33*a - 33, -9 = 3*a. Solve -105*p + 102*p - k = 0 for p.
-4
Let c be -511 - (-5 + 9 + -4 + 0). Let k = 524 + c. Solve 0 = -10*u + k*u + 3


443 S.E.2d 357 (1994)
114 N.C. App. 684
CONE MILLS CORPORATION, Appellee,
v.
ALLSTATE INSURANCE COMPANY, Appellant.
No. 9318SC349.
Court of Appeals of North Carolina.
May 17, 1994.
*359 Smith Helms Mulliss & Moore, by James A. Medford and Larissa Jones Erkman, Greensboro, for appellee.
Wilson & Iseman by G. Gray Wilson and Urs R. Gsteiger, Winston-Salem, for appellant.
MARTIN, Judge.
The parties advance several assignments and cross-assignments of error. The dispositive issue, however, is whether the trial court erred when it admitted evidence with respect to the intent of the parties and permitted the jury to determine whether the parties intended that the defense costs incurred in the Ostrander case would be included as part of the self-insured retention of $250,000.00 under the Northbrook policy. Both parties argue, and we agree, that the construction and application of thespinal cord injury at T5, we found a significant decrease in soma area of the SPNs in the segments below the site of injury: soma area of SPNs at T8 was 272.9+/-11 microm2. At T1 the soma area was 418+/-19 microm2. In the spinal cord obtained from a person who survived 23 years after cord injury at T3, the soma area of SPNs above (T1) and below (T7) the site of injury was similar (416.2+/-19 and 425.0+/-20 microm2 respectively). The findings demonstrate that the SPNs in spinal segments caudal to the level of the lesion undergo a significant decrease of their size 2 weeks after spinal cord injury resulting in complete transection of the spinal cord. The impaired cardiovascular control after spinal cord injury may be accounted for,


disease (CKD)47.8Malignancy00Chronic heart disease1529.4Hepatitis23.9Smoking HabitSmoker59.8Non-smoker4690.2Obesity35.9SignsPulse, Median (Q1-Q3)90(85-103)Temperature (°C), Median (Q1-Q3)37.5(37.1-38)Systolic blood pressure (mmHg), Median (Q1-Q3)124(113-136)Diastolic blood pressure (mmHg), Median (Q1-Q3)76(64-81)Respiration rate (rate of breathing), Median (Q1-Q3)20(20-23)

The vast majority 46 (90.2%) of the patients had pneumonia. Hematological findings on admission were normal; WBC 5 (3-7.38), Hb 13 mg/dl (11-15.1), and platelet 174 (134-263). The median and IQR of neutrophil and lymphocyte were 72.4 (59.5-83.4) and 22.4 (12.5-31.6), respectively. Of 51 positive MERS-CoV cases, 2 (3.9%) septic shock, 4 (7.8%) respiratory failure, and 1 (2%) multi-organic failure were reported as complications of the MERS-CoV infection. The median of time from illness onset to diagnosis was 8 days (5-10) while the time from illness onset to death due to MERS-CoV infection was 15 days (13-17.5). Therefore, the overall mortality rate wasthe time outbreaks are detected, and increased communication nationally and internationally have been critical in preventing international spread and sustained transmission \[[@bib0185]\].

Our study has the following limitations. First, the study design is a retrospective and was relied on chart review with some inherited issues; these involve missing data with respect the time course (from illness onset to hospital admission, diagnosis, death, and discharge from hospital). Second, some positive MERS-CoV cases might be sent from non-referral or private hospitals in our region to referral hospitals out Najran such as King Abdullah Medical Complex in Jeddah or Prince Muhammad bin Abdul Aziz Hospital in Riyadh; or mild cases may not come to our referral hospital, for these reasons, our study might have a selection bias. Although these limitations, we were


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+ O(\ups) \right ] \quad .
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%       && \quad + O(z^{2k}/r(1+\upz)^{2k+ 1/2}) + O(z^{2(k+m)}/r(1+\upz)^{2(k+m)+1/2} \}
% \quad ,
%\nonumber \\
\label{eq:strgresult}$$ The subleading terms in the potential will be obtained in a systematic expansion for small velocities and short distances valid down to distances of order $r_{\rm min.}^2$$=$$2\pi\alpha^{\prime} u$. They are succinctly expressed as a convergent power series in powers of the dimensionless variables, $z$$=$$r^2_{\rm min.}/r^2$, $\upz$, and $\ups$. Note that the potential is a quantum effect accounting for the fluctuations about the minimum action surface which determines the saddle point of the string path integral. It is time reversal invariant [@polchinskibook]: the power series only contains even powers of $u$. The numerical coefficient of the static term is a measureshort distances is from the massless modes in the open string spectrum. Restricting to these modes, we can express the potential as a double expansion in small velocities and short distances [@dkps] with the result: $$V(r,u) =  - {{{\rm tanh}(u)/u }\over{r(1+\upz)^{1/2}}}
   \left \{ (d-2)
{{{\mathbf{\gamma}}(\half, (\pi+ uz)/z )}\over{\Gamma (\half)}}
  + O(z^{2}/(1+\upz)^{2}) \right \} \quad ,
\label{eq:strgresultrect}$$ where $z$ is a dimensionless scale factor, $z$$=$$r^2_{\rm min.}/r^2$, and $r_{\rm min.}$ is the minimum distance that can be probed in the small velocity expansion at short distances [@bachas]: $r^2_{\rm min.}$$=$$2 \pi \alpha^{\prime} u$. ${\mathbf{\gamma}}(\half, (\pi+uz)/z )$ is the incomplete gamma function. The resummation and systematics of the small velocity expansion are discussed in Section IVA. The scale factor $z$ determines the magnitude of the velocity dependent


distances. The phase transition found in the large $d$ analysis of a class of phenomenological string models including the Nambu-Goto string [@alvarezstatic] appears to be a large $d$ artifact.

D0branes are point-like spacetime topological defects present in the generic background of the open and closed bosonic string theory. In section IVB, we note that the short distance potential between two static D0branes in bosonic string theory gives a linear interaction, $V_{\rm D0brane}$$=$$-(d-2)r/2\pi\alpha^{\prime}$. The static potential is the shift in the vacuum energy due to a constant background electromagnetic potential, but with vanishing electric field strength [@dbrane; @bachas; @polchinskibook]. The D0branes are assumed to have fixed spatial separation in the direction $X^{d-1}$, and to be in relative motion with nonrelativistic velocity $v$ in an orthogonal direction $X^d$ [@bachas; @dkps; @polchinskibook].The systematics of the small velocity short distance double expansion, and the value for the minimum distance probed in the scattering of D0branes, is identical to the results obtained in section IVA in general agreement with previous work.

The bosonic string has a tachyon, formally suppressed in obtaining this result, which must be stabilized in order to obtain a theory with a sensible ground state (see, for example, the recent discussion in [@sen]). Alternatively, it can be eliminated from the spectrum of physical states, as is possible in the fermionic type I and type II string theories [@polchinskibook]. Evidence for distance scales in String/M theory shorter than the string scale down to the eleven dimensional Planck length was originally observed in the form of the velocity dependent potential between


spacetime: $$\Sigma ~[X_{\mu}(\sigma^1) |_{(i,f)} ] ~=~
  {\tilde x}^{(i,f)}_{\mu}[f^{(i,f)}(\sigma^1)]
\quad\quad 0 \le \sigma^1 \le 1  \quad ,
\label{eq:repb}$$ Thus, the ${\tilde x}^{(i,f)} (\sigma^1 )$ are [*fiducial*]{} maps of the boundaries of the world sheet into the spacetime curves $C_i$, $C_f$, and the $f^{(i,f)}$ are arbitrary diffeomorphisms of $\sigma^1$ parameterizing the corresponding holes on the worldsheet.

The path integral sums over quantum fluctuations about a classical background determined by an extremum of the action. We look for minimum action configurations in the classical phase space of the Polyakov string. We separate each $X$ into a piece, ${\bar x}$, which solves the classical equation of motion with fiducial metric, ${\hat g}$, and assumes the functional form ${\tilde x}^{(i,f)}$ on the boundary, and a quantum fluctuation which satisfies the zero Dirichlet condition.loops of uniform radius $L/2\pi$ separated by a distance $R$. Align the circles parallel to the $X^p$, $X^{0}$ plane, with their axis in a perpendicular direction. Here $X^0$ is a Euclidean coordinate. The minimum area world-sheet is a catenoid [@kreyszig]: $${\bar x}= (a {\rm Cos}(2\pi\sigma^1), a {\rm Sin}(2\pi \sigma^1),
h(a)) , \quad\quad a^2 = (X^p)^2 +(X^{0})^2 \quad ,
\label{eq:catenoid}$$ with $L^{\prime}/2\pi$$\le$$a$$\le$$L/2\pi$. The radial parameter, $a$, is related to the height of the catenoid, $h(a)$, by the equation, $a$$=$$(L^{\prime}/2\pi) {\rm Cosh}(2\pi h(u)/L^{\prime})$. $L^{\prime}/2\pi$ is the minimum radius of cross-section for the catenoid. It is straightforward to evaluate the Polyakov action for this surface. Consider the maps that must be included in the sum over reparameterizations of the world-sheet boundary for this configuration of loops. In general, this is a


is computed with the zero Dirichlet boundary condition, and $l$ is the cylinder modulus defined by the fiducial metric, $ds^2$$=$$l^2(d\sigma^1)^2
$$+$$(d\sigma^2)^2$, $0$$\le$$\sigma^1$$\le$$1$, $0\le$$\sigma^2$$\le$$1$. With this choice, the area of the world-sheet is normalized to $l$.

Next consider the integration over metric deformations vanishing on the boundary. As in [@polyakov; @alvarez; @poltorus; @chaupath], we isolate the dependence on symmetric traceless variations of the metric and divide out by the volume of the gauge group $[{\rm Diff}_M]_0$, diffeomorphisms of the world-sheet continuously connected to the identity and vanishing on the boundary. Normalize the path integrations on the cylinder as in [@poltorus; @chaupath]: $$\int [d \delta {\hat g} ] e^{-|\delta {\hat g}|^2/2} \equiv
 \prod_{\sigma} \int [d \delta {\hat g} ]_{\sigma} e^{-|\delta
{\hat g}|_{\sigma}^2/2} = 1 =
 J_M({\cal \phi},{\hat g}) \int [don the boundary is cancelled against the volume of the gauge group $[{\rm Diff}_M]_0$. The result is an integral over the cylinder modulus times the quantum functional integral for Liouville field theory: $$% \int_0^{\infty}  {{d t}\over{t}} ({\rm Det}' \Delta_1)^{1/2}
J_M(\phi , {\hat g})
     \int [d \delta \phi ]_{e^\phi {\hat g}} ~ e^{-S_L[\phi,{\hat g}]
  - S_{\rm boundary}[\phi,{\hat e}]}
                 \quad ,
\label{eq:bulkm}$$ where $S_{\rm boundary}$ includes any boundary terms necessitated by the world-sheet gauge symmetries. $S_L[{\cal \phi},{\hat g}]$ is the unrenormalized Liouville action [@polyakov]: $$S_L[\phi,{\hat g}] = {{d - 26}\over{48 \pi}}
\int_M d^2 \sigma {\sqrt {\hat g}} [ \half {\hat g}^{ab}
   \partial_a \phi \partial_b


spatial separation $b$ in the direction $X^{d-1}$, and are in relative slow motion in an orthogonal direction $X^d$ with velocity $v$ [@bachas]. At long distances their static interaction potential will take the Newtonian form. The effective potential at long distances is dominated by the exchange of the lowest lying states in the [*closed*]{} string spectrum. With no loss of generality, we can obtain the potential between two D0branes as a special case of the general expression for the scattering of two Dpbranes, $p$$<$$d$. We will show that the systematics of the small velocity short distance double expansion and the value for the minimum distance probed in the scattering, $r_{\rm min.}$, is identical to the result obtained above, in general agreement with previous analyses [@bachas; @dkps; @polchinskibook].

Adapting the computationthis result which will be explored in forthcoming work [@typeI]. We have demonstrated the validity of the double expansion in small velocities and short distances down to a minimum distance, $r^2_{\rm min.}$$=$$2\pi\alpha^{\prime}u$, in general agreement with previous estimates [@shenker; @bachas; @dkps; @polchinskibook]. Thus, String/M theory predicts an [*infinite*]{} number of velocity dependent corrections to the potential between two heavy sources in relative slow motion in a gauge theory, the numerical coefficients of which are predicted by a systematic expansion. We are not aware of a comparable theoretical analysis which reliably probes this regime of QCD. We note that there is no evidence of non-analytic behavior in the potential between sources at short distances, suggesting that the phase transition at short distances previously found in [@alvarezstatic; @durhuus] is a


large $d$ artifact.

The numerical difference between the coefficient of the $1/r$ term we have found in the static potential at short distance and that given by Lüscher’s effective field theory analysis for the QCD flux tube valid at long distance scales deserves explanation. We should note that the flux tube picture is inherently a long distance concept whose predictions cannot be naively extrapolated to short distances. Consider the $d=26$ dimensional bosonic string. At both long and short distances there is a proportionality factor in the $1/r$ potential which equals $d-2$, the number of transverse massless gluon modes. The short distance static potential between heavy point sources in the gauge theory is a measure of fluctuations in the vacuum energy density. It would be gratifying if one could exploitsummary judgment on the issue of liability because there are no relevant contested issues of fact in this regard and that Morvant has violated the statute and is entitled to judgment as a matter of law. Morvant has filed in effect a cross-motion with respect to liability. Moreover, Morvant also contends that "if this Honorable Court rules that in fact the Act prohibited Dr. Morvant's referrals of Mr. Hodgkinson and Mr. Pena, the Act itself is unconstitutional in prohibiting these referrals." To that end Dr. Morvant seeks to dismiss the suit "for lack of subject matter jurisdiction."
The facts that brought rise to this suit are as follows:

Ismael Pena
Ismael Pena and his partner, Patrick Dunne, were longstanding patients of Morvant's. According to the deposition testimony of Dunne and the


limitations under the License.
 */

package org.apache.gobblin.runtime.spec_serde;

import java.lang.reflect.Type;
import java.net.URI;

import com.google.gson.JsonArray;
import com.google.gson.JsonElement;
import com.google.gson.JsonObject;
import com.google.gson.JsonSerializationContext;
import com.google.gson.JsonSerializer;
import com.typesafe.config.ConfigRenderOptions;

import org.apache.gobblin.runtime.api.FlowSpec;
import org.apache.gobblin.runtime.api.Spec;

public class FlowSpecSerializer implements JsonSerializer<FlowSpec> {
  public static final String FLOW_SPEC_URI_KEY= "uri";
  public static final String FLOW_SPEC_VERSION_KEY = "version";
  public static final String FLOW_SPEC_DESCRIPTION_KEY = "description";
  public static final String FLOW_SPEC_CONFIG_KEY = "config";
  public static final String FLOW_SPEC_CONFIG_AS_PROPERTIES_KEY = "configAsProperties";
  public static final String FLOW_SPEC_TEMPLATE_URIS_KEY = "templateURIs";
  public static final String FLOW_SPEC_CHILD_SPECS_KEY = "childSpecs";

  @Override
  public JsonElement serialize(FlowSpec src, Type typeOfSrc, JsonSerializationContext context) {
    JsonObject flowSpecJson = new JsonObject();

    flowSpecJson.add(FLOW_SPEC_URI_KEY, context.serialize(src.getUri()));
    flowSpecJson.add(FLOW_SPEC_VERSION_KEY, context.serialize(src.getVersion()));
    flowSpecJson.add(FLOW_SPEC_DESCRIPTION_KEY, context.serialize(src.getDescription()));
    flowSpecJson.add(FLOW_SPEC_CONFIG_KEY, context.serialize(src.getConfig().root().render(ConfigRenderOptions.concise())));

    flowSpecJson.add(FLOW_SPEC_CONFIG_AS_PROPERTIES_KEY, context.serialize(src.getConfigAsProperties()));

    JsonArray templateURIs = newsolution is expensive since particularly large contact areas are required.
The prior art likewise discloses using guide systems in order to preclude malfunctions of the switch pole from the outset for the purpose of avoiding incorrect orientations of the kind. Additional components and structural elements which are fitted to the pole shell, such as special guide bearings for example, are used for this purpose, as a result of which the structural design of the switch pole becomes comparatively complex.


the confusion Bockwinkel won the match. The Lawler/Kaufman feud ended in the early part of 1983 after Lawler threw a fireball at Kaufman, ending his run with the CWA. After Kaufman left, Lawler refocused his efforts on Jimmy Hart and his First Family stable.

Lawler challenging for the World title and almost winning it was a recurring theme throughout the mid-1980s, with neither the AWA nor the NWA being willing to actually put their main title on Lawler. The NWA World title was not defended very often in the Memphis area, usually touring with companies that had more political clout in the Alliance, which meant that the CWA actually featured the AWA World champion more regularly than the group of which they were actually dues-paying members.

In 1988, plans wereitself in a minority position in the company, in which a partnership is being forced on it with known real estate sharks," the moshav states in its petition, and mentions that there is an agreement between Mega Or and the Bronfman-Fisher partnership to buy the land in order to construct IKEA branches in Israel, and that an IKEA branch was built in Beer Sheva on this format, among other things.

Indeed the moshav claims in its petition that the parties combined with lack of good faith in order to deny the moshav's basic refusal right, with Barazani gaining a huge profit and the new buyers forcing themselves on the moshav, while at the same time initiating press reports about the construction of an IKEA branch on Eshtaol's land in


order to create an accomplished fact, while ignoring the moshav's rights. "This is an extremely grave act, because even if this partnership had some right in the company, the rental agreement between the company and another company (IKEA) is clearly a party at interest transaction requiring the moshav's consent. The buyers are therefore treating the moshav as if it were air."

RELATED ARTICLES

Last January, a meeting took place between representatives of the moshav and the new buyers, at which it was made clear to the buyers that the moshav had not waived its refusal right, and that the sale of shares in the industrial park company could not be completed without the moshav's consent. In addition, the representatives made it clear that there was a possibility of the buyersQ:

Counter in VHDL

Designing a counter mod60 in VHDL, I realized that something strange happens, but I can't explain why.
This image shows the moment of the transition from 59 to 00 (numbers converted to a 7SegDisp):

The code for it is:
ENTITY Contador IS  --"Contador" means counter
    PORT(
        clk: IN BIT;
        disp_uni, disp_dez: OUT BIT_VECTOR (6 DOWNTO 0)
    );
END Contador;
--------------------
ARCHITECTURE Contador OF Contador IS
    ------
    SIGNAL unidade: NATURAL RANGE 0 TO 10; --units
    SIGNAL  dezena:  NATURAL RANGE 0 TO 6; --tens

    COMPONENT ConvDisp IS
        --display conversor's entity goes here


cerebellum, has been postulated. Increased thresholds for the excitation of the hand-associated motor cortex contralateral to the cerebellar lesion correlated with slow and clumsy finger movements ipsilateral to the cerebellar lesion, which suggests facilitatory influences of the cerebellum on the contralateral corticospinal system under normal conditions.fact that he experienced no difficulty in securing and retaining another position at a higher salary, but also by plaintiff's own testimony that he was unable to hire a satisfactory substitute. Defendant did not claim that he was required to render services other than those in his original contract with plaintiff in order to obtain a higher salary from his new employer, nor did plaintiff prove by expert testimony how much such services would bring in the market. But plaintiff did prove the amount defendant actually received. Under such circumstances, there was some evidence of the value of defendant's services and therefore of the cost of replacement. As was said in Triangle Waist Co. v. Todd, 223 N.Y. 27, 119 N.E. 85, 86:
"* * * If one agrees


Diuron treatment reveals the different roles of two cyclic electron transfer pathways in photosystem II in Arabidopsis thaliana.
Three ecotypes of Arabidopsis thaliana, ecotype Columbia (Wild type, Wt) and two mutants (pgr5 and ndf4), were used to evaluate the effects of diuron on photosynthetic activity of A. thaliana. It was found that diuron adversely affected the fresh weight and chlorophyll content of the plants. Chlorophyll fluorescence studies determined that the pgr5 mutant was more sensitive to diuron than Wt and the ndf4 mutant. Gene expression analysis revealed different roles for the two cyclic electron transfer (CET) pathways, NAD(P)H dehydrogenase (NDH) and proton gradient regulation (PGR5) pathways, in the plant after diuron treatment. For example, a gene in the NDH pathway, lhca5, was activated in the low dose (LD) groupexplicitly located in both structures, unambiguously confirming the successful isolation of the cis porphyrin tautomer. Given the rather unusual substitution patterns of these two porphyrins, which are rather inaccessible from a synthetic point of view, we were interested in finding cis tautomers among more readily available free-base porphyrins. Accordingly, we turned our attention to free-base β-octabromo-*meso*-tetraphenylporphyrins,^[@ref8],[@ref9]^ which can be synthesized quite straightforwardly, a strategy that proved rewarding. We obtained single-crystal X-ray structures of two such porphyrins as bis-methanol adducts, namely, 2,3,7,8,12,13,17,18-octabromo-5,10,15,20-tetrakis(4**′**-trifluoromethylphenyl)porphyrin, H~2~\[Br~8~TCF~3~PP\]·2CH~3~OH,^[@ref10]^ and 2,3,7,8,12,13,17,18-octabromo-5,10,15,20-tetrakis(4**′**-fluorophenyl)porphyrin, H~2~\[Br~8~TFPP\]·2CH~3~OH. Although the central hydrogens in the two structures could not all be unambiguously located, they nonetheless could be convincingly modeled as porphyrin cis tautomers ([Table [1](#tbl1){ref-type="other"}](#tbl1){ref-type="other"}). Furthermore, a perusal of the Cambridge Structural Database (CSD)^[@ref11]^ suggests that there may well be additional examples


H~2~\[Br~8~TCF~3~PP\]·2CH~3~OH.](ao0c00517_0001){#fig3}

![Simplified schematic representation of the two structures obtained in this work. The four nitrogen atoms connected by solid lines represent the saddle-shaped porphyrin. The two CH~3~OH solvent molecules are poised directly above and below the porphyrin, with each methanol oxygen within hydrogen-bonding distance of a pair of trans nitrogen atoms of the porphyrin. (a) Depiction of the hydrogen-bonding network in H~2~\[Br~8~TCF~3~PP\]·2CH~3~OH modeled as an ordered cis tautomer. (b) Disorder model in H~2~\[Br~8~TFPP\]·2CH~3~OH. Atoms in purple are at 50% occupancy. Careful analysis of the disorder is necessary to deduce chemically reasonable hydrogen-bonding networks.](ao0c00517_0002){#fig4}

###### Hydrogen-Bond Geometries (Å and deg)

  D--H···A                             as a free base porphyrin (assuming a p*K*~b~ similar to pyridine, i.e., ∼5) is not expected to deprotonate a weak acid such as methanol (p*K*~a~ = 15.5).

The reader may find it useful to explicitly consider the possible hydrogen-bonding networks for porphyrin trans tautomers. [Figure [5](#fig5){ref-type="fig"}](#fig5){ref-type="fig"}a depicts two equally contributing structures that average to give the disorder model shown in [Figure [4](#fig4){ref-type="fig"}](#fig4){ref-type="fig"}b. In this model, a hydrogen-bond network is generated by protonating one methanol to give CH~3~OH~2~^+^ and deprotonating another methanol to give CH~3~O^--^, an unlikely scenario that we deemed chemically unreasonable. [Figure [5](#fig5){ref-type="fig"}](#fig5){ref-type="fig"}b shows two of the four equally contributing conformations that also average to give the disorder model in [Figure [4](#fig4){ref-type="fig"}](#fig4){ref-type="fig"}b. In this model, the methanol on the "protonated" face of the saddled *trans* tautomer acts as


[6](#fig6){ref-type="fig"}](#fig6){ref-type="fig"} depicts four equally contributing conformations of a porphyrin cis tautomer that average to give the disorder model depicted in [Figure [4](#fig4){ref-type="fig"}](#fig4){ref-type="fig"}b. Each conformation gives a reasonable hydrogen-bonding motif with neutral methanol to form the transannular N--H···X--H···N hydrogen-bonding network proposed in our earlier work.

![Four equally contributing conformations for H~2~\[Br~8~TFPP\]·2CH~3~OH. Disordered groups, each at 50% occupancy, are shown in purple. The cis tautomer is the only form that gives a chemically reasonable hydrogen-bonding model with neutral methanol. Upon averaging, the four structures depicted above give the disorder model shown in [Figure [4](#fig4){ref-type="fig"}](#fig4){ref-type="fig"}b.](ao0c00517_0007){#fig6}

A longstanding observation worth recalling in this connection is that the C~α~--N--C~α~ angles serve as an indirect but quite reliable probe of the *N*-protonation sites in free-base porphyrins, with unprotonated pyrrole groups exhibiting C~α~--N--C~α~ angles in the 106--108°range and protonated pyrrole groups exhibiting C~α~--N--C~α~ angles in the 110--112° range.^[@ref14]−[@ref20]^ For the two crystallographically unique molecules of H~2~\[Br~8~TCF~3~PP\]·2CH~3~OH, the angles for the putative protonated pyrrole rings are 111.0(3), 111.0(3), 111.3(4), and 110.5(4)° and those for putative unprotonated pyrrole rings are 107.4(4), 107.4(3), 107.8(4), and 107.2(4)°, in excellent agreement with structural precedent. For H~2~\[Br~8~TFPP\]·2CH~3~OH, the C~α~--N--C~α~ angle is 109.0(5)°, a reasonable value considering that the disorder model entails an averaging of two protonated and two unprotonated pyrrole rings.

With four porphyrin cis tautomers documented by us (including the two here), a question that begs to be answered is "how many more might there be in the literature?". This question proved more difficult to answer than expected for multiple reasons. First, the N--H hydrogen-atom positions are often difficult or


8453 spectrophotometer in CH~2~Cl~2~ at room temperature. NMR spectra were recorded on a Mercury Plus Varian spectrometer (400 MHz for ^1^H and 376 MHz for ^19^F) at 298 K. ^19^F shifts (δ) in ppm were referenced to 2,2,2-trifluoroethanol-*d*~3~ (δ = −77.8 ppm). Mass spectra were recorded on a Waters Micromass matrix-assisted laser desorption/ionization (MALDI) Micro MX mass spectrometer with *α*-cyano-4-hydroxycinnamic acid as the matrix.

Syntheses {#sec4.2}
---------

*Meso*-tetrakis(4-fluorophenyl)porphyrin, H~2~\[TFPP\], and *meso*-tetrakis(4-trifluoromethylphenyl)porphyrin, H~2~\[TCF~3~PP\], were synthesized via modified^[@ref29],[@ref30]^ Adler--Longo^[@ref31]^ procedures. The corresponding Cu complexes were prepared by refluxing the free bases overnight with Cu(OAc)~2~·H~2~O (10 equiv) in DMF and purified via flash chromatography as described for copper tetraphenylporphyrin.^[@ref32]^ The copper octabromoporphyrins Cu\[Br~8~TXPP\] (X = F, CF~3~) were prepared following a literature protocol.^[@ref33]^ To obtain Cu\[Br~8~TFPP\], Cu\[TFPP\] was brominated in CHCl~3~ with 24 equivinnings. Just as it looked as though his time had surely past, Pakistan's team management stood firmly behind Kamran, and his younger brother Umar - the only alternative behind the stumps - picked up a finger injury. There are doubts over whether Umar will play, even just as a batsman, which would deprive Pakistan of their second-highest run-scorer in the tournament and means they are likely to persist with the eight-batsman strategy. Up against a Zimbabwe side that has failed to match the scrapping resilience of some of their past World Cup outfits, Pakistan can expect an immediate revival in their fortunes. A win would take them to eight points, level with New Zealand in the Group A table.

Form guide

Pakistan LWWWLZimbabwe LLWLL

Watch out for...

Among the carnage that was


Asad Shafiq, while Ahmed Shehzad can expect to hold his place despite making 36 runs from his four outings. Shoaib Akhtar's woeful effort against New Zealand will prompt calls for Wahab Riaz's inclusion.

Pallekelle has not quite matched Bangalore for gratuitous run-fests but has certainly aided the batsmen in its few games so far. Ross Taylor found the boundaries small enough to clear seven times in his unbeaten 131 against Pakistan and Sri Lanka coasted to 327 against Zimbabwe last Thursday. It's harder for the team batting second under lights, so the toss is important.

Stats

In four World Cup meetings between the sides Pakistan have won three with the Bulawayo tie in 2003 being rained off.

The 349 Pakistan made against Zimbabwe in Kingston in 2007 is their highest World CupSubstrates that include one or more layers of semiconductor material are used to form a wide variety of semiconductor structures and devices including, for example, integrated circuit (IC) devices (e.g., logic processors and memory devices), radiation emitting devices (e.g., light emitting diodes (LEDs), resonant cavity light emitting diodes (RCLEDs), and vertical cavity surface emitting lasers (VCSELs)), and radiation sensing devices (e.g., optical sensors). Such semiconductor devices are conventionally formed in a layer-by-layer manner (i.e., lithographically) on and/or in a surface of a semiconductor substrate.
Historically, a majority of such semiconductor substrates that have been used in the semiconductor device manufacturing industry have comprised thin discs or “wafers” of silicon material. Such wafers of silicon material are fabricated by first forming a large, generally cylindrical, silicon single-crystal ingot and subsequently


as a “handle” or “handling” substrate. The base substrate may also comprise a semiconductor material.
A wide variety of engineered substrates are known in the art and may include semiconductor materials such as, for example, silicon (Si), germanium (Ge), III-V type semiconductor materials, and II-VI type semiconductor materials. For example, an engineered substrate may include an epitaxial layer of III-V type semiconductor material formed on a surface of a base substrate, such as, for example, aluminum oxide (Al2O3) (which may be referred to as “sapphire”). Using such an engineered substrate, additional layers of material may be formed and processed (e.g., patterned) over the epitaxial layer of III-V type semiconductor material to form one or more devices on the engineered substrate.
Due to a natural tendency of atoms of different material20?
False
Is 1508 a multiple of 36?
False
Does 52 divide 3900?
True
Does 7 divide 532?
True
Is 3724 a multiple of 14?
True
Is 455 a multiple of 5?
True
Does 153 divide 635?
False
Does 9 divide 369?
True
Is 480 a multiple of 15?
True
Is 6336 a multiple of 88?
True
Is 38916 a multiple of 23?
True
Is 8010 a multiple of 15?
True
Is 2 a factor of 5569?
False
Does 2 divide 419?
False
Does 38 divide 10526?
True
Does 416 divide 74880?
True
Is 6 a factor of 375?
False
Is 1045 a multiple of 15?
False
Is 47 a factor of 188?
True
Is 11503 a multiple of 8?
False
Does 70 divide 3500?
True
Is 69 a factor of 1219?
False
Is 49 a factor of 4568?
False
Is 63 a factor of 52353?
True
Is 37 a factor of 2923?
True
Is 6099 a multiple of 20?
False
Is 1343 a multiple of 46?
False
Does 13 divide 3685?
False
Is 25 a factor of 53075?
True
Is 17 a factor of 2402?
False
Is


the clinical complex of signs; case histories are given in detail as examples. Since pathologico-anatomically identified severe arteriosclerotic changes of the long medullary arteries are most probably the cause of the hypoxically conditioned diffuse vacuolous demyelinisation of the medullary layer, computerised tomography yields an important indirect pointer to the condition of the cerebral vascular periphery. This additional information seems to be important in arriving at an indication for invasive diagnostic or surgical procedures relating to the vascular system.career in the building materials industry, serving in various positions with local and national manufacturers, primarily in kitchen design and sales.

Senate Committees

 Transportation, Minority Spokesperson
 Appropriations II
 Education
 Energy
 Revenue
 Gaming

Personal life
Don is married to his wife Diane, and together they have two children. The DeWittes are lifelong members of St. Patrick Church in St. Charles, and regularly support two local non-profits, Lazarus House in St. Charles and CASA Kane County.

References

External links
Senator Donald P. DeWitte (R) 33rd District at the Illinois General Assembly
By session: 100th, 101st

Category:Illinois state senators
Category:Illinois Republicans
Category:Living people
Category:21st-century American politicians
Category:People from St. Charles, Illinois
Category:Year of birth missing (living people)


allelic states (i.e. heterozygous and homozygous) were used simultaneously as explanatory variables so that the results are relative to the wild type genotype (Table [1](#Tab1){ref-type="table"}). We tested for an association between each polymorphism and expression levels of five markers of the parasite *var* gene expression profile that tend to be differentially associated with host immunity: i) the overall proportion of expressed *var* gene sequences that are classified as cys2 and, ii) the proportion of cys2 *var* genes that fall in the MFK + REY-, iii) MFK-REY+, iv) MFK-REY- or v) group A-like subgroup. Our aim was to determine whether host polymorphism have an independent effect on *var* gene expression and hence all regression models were adjusted for covariates previously found to be associated with cys2 *var* gene expression levels in the***p***valueBeta (95% CI), ***p***valueBeta (95% CI), ***p***valueABO blood groupBlood group O, 10800000Blood group A, 760.004 (-0.10, 0.11), *p* = 0.9-0.004 (-0.10, 0.09), *p* = 0.9-0.004 (-0.09, 0.08), *p* = 0.90.01 (-0.07, 0.09), *p* = 0.8-0.01 (-0.09, 0.06), *p* = 0.7Blood group B, 540.05 (-0.07, 0.16), *p* = 0.40.08 (-0.02, 0.19), *p* = 0.10.08 (-0.02, 0.17), *p* = 0.10.01 (-0.08, 0.09), *p* = 0.8-0.01 (-0.09, 0.07), *p* = 0.8Blood group AB, 120.13 (-0.08, 0.34), *p* = 0.20.25 (0.07, 0.44), *p* = 0.0080.07 (-0.10, 0.24), *p* = 0.40.06 (-0.10, 0.21), *p* = 0.50.02 (-0.12, 0.17), *p* = 0.8CD36 (T188G)Wild type (T/T), 15300000Heterozygous (T/G), 220.08 (-0.06, 0.23), *p* = 0.30.03 (-0.10, 0.15), *p* = 0.70.03 (-0.08, 0.14), *p* = 0.6-0.01 (-0.12, 0.11), *p* = 0.90.07 (-0.04, 0.18), *p* = 0.2Homozygous (G/G), 1NDNDNDNDNDICAM1 (K29M)Wild type (K29/K29), 7900000Heterozygous (K29/M29), 74-0.03 (-0.13, 0.07), *p* = 0.6-0.07 (-0.16, 0.02), *p* = 0.1-0.03 (-0.11, 0.05), *p* = 0.40.04 (-0.04, 0.12), *p* = 0.3-0.06 (-0.14, 0.01), *p* = 0.1Homozygous (M29/M29), 23-0.05 (-0.21, 0.10), *p* = 0.5-0.01 (-0.15, 0.12), *p* = 0.90.06 (-0.06, 0.17), *p* = 0.3-0.07 (-0.20, 0.05), *p* = 0.2-0.09 (-0.20, 0.03), *p* = 0.1HbSWild type


The association between carriage of the blood group AB and high group A-like *var* gene expression is thus consistent with the fact that parasite isolates from children with severe malaria tend to express higher levels of group A-like *var* genes \[[@CR7], [@CR27]--[@CR29]\]. In our dataset, parasite rosetting, defined as the spontaneous binding of infected to uninfected erythrocytes, was strongly correlated with group A-like *var* expression (N = 133, rho = 0.46, *p* \< 0.0001; \[[@CR14]\]). However, despite the observed association between blood group AB and high group A-like *var* expression (Table [1](#Tab1){ref-type="table"}), among isolates with rosetting data available (N = 133) parasite rosetting frequency only correlated with blood groups A (Beta = 0.12, 95% CI 0.005, 0.24, *p* = 0.04) and B (Beta = 0.18, 95% CI 0.04, 0.31, *p* = 0.01), but not AB (Beta = 0.04, 95% CI -0.18, 0.25, *p* = 0.7) in a regression analysisExercise 2], we get that all the one dimensional projections of the $\mu^y$ are Gaussian, thus $\mu^y$ is a Gaussian measure in ${\mathcal{X}}$, $\mu^y={\mathcal{N}}(\overline{m},\overline{{\mathcal{C}}})$ for some $\overline{m}\in{\mathcal{X}}$ and a self-adjoint, positive semi definite, trace class linear operator $\overline{{\mathcal{C}}}$. It suffices to show that $\overline{m}=m$ and $\overline{{\mathcal{C}}}={\mathcal{C}}$.

We use the standard Galerkin method to show that $m^N\to m$ in ${\mathcal{X}}$. Indeed, since by their definition $m^N$ solve (\[eq:int7\]) in the $N$-dimensional spaces ${\mathcal{X}}^N$, for $e=m-m^N$, we have that $B(e,v)=0, \;\forall v\in {\mathcal{X}}^{N}$. By the coercivity and the continuity of $B$ (see Proposition \[laxmil\])$${\big\|e\big\|}_1^2\leq cB(e,e)=cB(e,m-z)\leq c{\big\|e\big\|}_1{\big\|m-z\big\|}_1, \;\forall z\in{\mathcal{X}}^N.\nonumber$$ Choose $z=P^Nm$ to obtain $${\big\|m-m^N\big\|}\leq c{\big\|m-P^Nm\big\|}_1,\nonumber$$ where as $N\to\infty$ the right hand side converges to zero since $m\in X^1$. On the other hand, by [@MR1642391 Example 3.8.15], we have that $m^N\to\overline{m}$ in ${\mathcal{X}}$, hence


that ${\mathcal{A}}_0=-\boldsymbol{\Delta}$, we have by the product rule for derivatives that ${\mathcal{A}}_0^\kappa\mathcal{M}_w{\mathcal{A}}_0^{-\kappa}$ is bounded, provided $w\in W^{2\kappa,\infty}(\Omega)$.

The operators $K_i$ are compact in ${\mathcal{X}}$, since they are compositions between the compact operator ${\mathcal{A}}_0^{-s}$ and the bounded operator ${\mathcal{A}}_0^{t}\mathcal{M}_w{\mathcal{A}}_0^{-t}$. Positivity of the operator ${\mathcal{A}}_0$ and nonnegativity of the operator $\mathcal{M}_w$ show that $-1$ cannot be an eigenvalue of $K_i$, so that by the Fredholm Alternative [@MR0243367 27, Theorem 7] we have that $(I+K_i)^{-1}, i=1,2,$ are bounded in ${\mathcal{X}}$.

The Diagonal Case {#sec:diag}
=================

In the case where ${\mathcal{C}}_0, {\mathcal{C}}_1$ and ${\mathcal{A}}$, are all diagonalizable in the same eigenbasis our assumptions are trivially satisfied, provided $\Delta>2s_0$. In [@1232.62079], sharp convergence rates are obtained for the convergence in (\[eq:main1\]), in the case where the three relevant operators are simultaneously diagonalizable and have spectra that decay algebraically; thewe required a certain degree of ill-posedness compared to the regularity of the prior (Assumption \[a2\](\[a2delta\])) and for the convergence rates to be valid a certain degree of regularity of the true solution. In the case where the three involved operators are all diagonalizable in the same eigenbasis, when the problem is sufficiently ill-posed with respect to the prior, and for a range of values of $\gamma$, the parameter expressing the regularity of the true solution, our rates agree (up to $\varepsilon>0$ arbitrarily small) with the sharp (minimax) convergence rates obtained in [@1232.62079] (Section \[sec:diag\]).

Our optimized rates rely on rescaling the prior depending on the size of the noise, achieved by choosing the scaling parameter $\tau^2$ in the prior covariance as an appropriate function of the parameter $n^{-\frac12}$ multiplying


the prior, which are shown to give optimal rates up to slowly varying terms. We currently investigate hierarchical methods with conjugate priors and hyperpriors for data driven choices of both the scaling parameter of the prior $\tau$ and the noise level $n^{-\frac12}$.

The methodology presented in this paper is extended to drift estimation for diffusion processes in [@Pokern:2012fk]. Future research includes the extension to an abstract setting which includes both the present paper and [@Pokern:2012fk] as special cases. Other possible directions are the consideration of nonlinear inverse problems, the use of non-Gaussian priors and/or noise and the extension of the credibility analysis presented in [@1232.62079] to a more general setting.

[25]{} natexlab\#1[\#1]{}\[2\][\#2]{} , , (). , , , , volume  of **, , , . . , , , volume  of **, ,code from it:
(defun tina/test-finalize ()
  (let ((key  (plist-get org-capture-plist :key))
        (desc (plist-get org-capture-plist :description)))
    (if org-note-abort
        (message "Template with key %s and description “%s” aborted" key desc)
      (message "Template with key %s and description “%s” run successfully" key desc))))

(add-hook 'org-capture-after-finalize-hook 'tina/test-finalize)

So, wrapping your function in a test like (when (and (not org-note-abort) (equal (plist-get org-capture-plist :key) "g")) … ) should do the trick!

A:

The solution by Tina Russell is probably the way to go (did not try it). I solved it using the code below.
  (defun clean-up-template ()
    "Remove all unchecked items in the checklist"
    (if (org-entry-get (point-min)


worked perfectly.

A:

Three errors.

1. The following create an array with one element, a reference to a hash:
my @array = {"foo", "bar", "poo"};

You surely meant to use
my @array = ("foo", "bar", "poo");

2.
$hash->{mykey} = @array;

is the same thing as
$hash->{mykey} = 3;

You can't store arrays in scalars, but you can store a reference to one.
$hash->{mykey} = \@array;

3.  It would be
rand(@a)    # rand conveniently imposes a scalar context.

for an array, so it's
rand(@{ $ref })

for a reference to an array. That means you want the following:
my $element = $hash->{mykey}[ rand(@{ $hash->{mykey} }) ];

Or you can break it down into two lines.
my $array = $hash->{mykey};
my $element = $array->[ rand(@$array) ];

All together, we have the following:
my @array = ( "foo", "bar", "poo" );
my $hash = { mykey => \@array };

my $element      [SecurityCritical]
        public static AppDomain GetDefaultAppDomain()
        {
            (new PermissionSet(PermissionState.Unrestricted)).Assert();
            if (AppDomain.CurrentDomain.IsDefaultAppDomain())
            {
                return AppDomain.CurrentDomain;
            }
            var isMono = Type.GetType("Mono.Runtime") != null;
            if (isMono)


Associated Press

LAS VEGAS - Republican Nevada state Assemblywoman Michele Fiore has filed paperwork to run for Congress.

Fiore registered Wednesday with Clark County to get her name on the November ballot.

She’s seeking to represent southern Nevada’s 3rd Congressional District, covering the Summerlin area of northwest Las Vegas and Henderson.

Republican Rep. Joe Heck holds the seat, but is running for U.S. Senate.

Fiore is an outspoken, two-term state lawmaker best known for her love of guns, support for Nevada rancher Cliven Bundy and her recent intervention to coax the last remaining occupier from a federal wildlife refuge in Oregon.

The congressional race to replace Heck is crowded with Republican contenders, including Nevada Senate Majority Leader Michael Roberson, unsuccessful 2012 congressional candidate Danny Tarkanian and former Nevada Policy Research Institute executive Andy Matthews.Monero is a secure, private, and untraceable cryptocurrency. It is open-source and accessible to all.

It is the leader in Privacy Coins in the Cryto-currency space.

Im not sure I need to go into too much detail regarding the chart below…

It is very clear that the coin is very resilient to wider market macro and micro News/FUD/Regulatory Impact.

It appears to be reaching a Resistance/Support at $260.

If it falls below this then the next target could be the Trend Line bounce at around $200.


geodesic flow on the corresponding surface $\mathcal{S}_P$. In fact, as is explained in §\[subsec:singularities\], vertices constitute singularities of the billiard map and certain copies of the vertices in $\mathcal{S}_P$ constitute singularities of the flow on the surface. We discuss what implications this has for the billiard ball dynamics.

In §\[subsec:KSNratbilliard\], we view the prefractal polygonal billiard $KS_n$ as a rational billiard, and discuss the consequences of this fact for the billiard flow at the vertices of $KS_n$. We also construct the corresponding surface for $KS_1$, $KS_2$ and $KS_3$ and indicate the singularities of each surface. We show that, in agreement with the general theory of rational billiards, reflection at acute angles can be defined, but that reflection at obtuse angles cannot be determined unambiguously.

In the last part of Sectionrole in motivating and guiding our investigations on the ‘Koch snowflake billiard’ (and its rational polygonal approximations) reported in the present paper.

Flows on Rational Billiards and Corresponding Surfaces
======================================================

In this section, we want to discuss the properties of the billiard flow on $KS_n$ and describe how $KS_n$ can be viewed naturally as a *rational billiard*. A *rational polygon* is a polygon with interior angles that are rational multiples of $\pi$. If the boundary of a polygonal billiard is a rational polygon, then we call the associated billiard a *rational billiard*. For us to discuss the flow on the associated closed surface, we need to define a few concepts.[^8]

If $H$ is a regular $N$-gon, where $N$ is a positive integer, then $D_N$ is the group of symmetries of $H$ and


are coprime positive integers and $r$ is the number of vertices of $P$, then $G(P)$ is isomorphic to the dihedral group $D_N$, where $N$ is the least common multiple of $n_1,n_2,...,n_r$. \[prop:altDefinitionOfRatPolygon\]

If $P$ is a rational billiard, then we have at our disposal a method for discerning periodic orbits. This method was first given in [@KaZe] and reiterated in various forms in the literature; see, e.g., the survey articles [@GaStVo], [@Gu], [@MaTa] and [@Zo]. Let $x_0$ be the initial position of the billiard ball and $\theta_0$ be the initial direction of the billiard ball. Let $x_1$ be the point on the side $s_1$ of the billiard table at which the billiard ball collides, and $\theta_1$ be the angle at which the billiard ball reflects off of $s_1$. Ifthe associated generalized polygon is an octagon. Pairs of appropriate sides should be identified as indicated, in order to obtain $\mathcal{S}_P$, a surface of genus $g=2$. Note, however, that strictly speaking, this planar representation is not valid. We illustrate such an embedding here as a heuristic device.[]{data-label="fig:octagonsurface"}](octagonsurface.png)

The surface $\mathcal{S}_P$ is often referred to as a ‘translation surface’ or a ‘flat surface’ in the literature; see, e.g., [@Ve3], [@HuSc], [@MaTa], [@Vo] and [@Zo]. Indeed, the geodesic flow on $\mathcal{S}_P$ is nothing but the straight-line flow in the associated generalized polygon, with pairs of opposite sides identified as indicated above. The key fact concerning the geodesic flow on $\mathcal{S}_P$ is that it is (dynamically) equivalent to the billiard flow on $P$.

Singularities of the billiard flow on $P$ and of the


flat surfaces and can be viewed as the first three prefractal approximations of the ‘fractal flat surface’ (of infinite genus) $\mathcal{S}_{KS}$, which we will conjecture (in Section \[sec:conjectures\]) to exist as a proper mathematical object; see part (i) of Conjecture \[conj:fractalbilliardFractalSurface\].

Equilateral triangle billiards and implications for $\mathbf{KS_n}$. {#subsec:baum}
--------------------------------------------------------------------

The equilateral triangle billiard $\Delta$ is a very nice rational billiard. The billiard dynamics on $\Delta$ are well understood. Two orbits of an equilateral triangle billiard are said to be *equivalent* if each orbit has an unfolding that is a translate of the other and each have the same length. Denote the equivalence class of an orbit $\alpha$ by $[\alpha]$. In [@BaUm], Baxter and Umble give a classification of the periodic orbits of $\Delta$, up to this notion of equivalence. Roughly speaking, theybase $s_{0,1}$ of $\Delta = KS_0$ is given by $g_{0,1}=(1/3,2/3)$; see Fig. \[fig:illustrateDefis\](a).

\[def:compatiblesequence\] For each $n\geq 0$, let $\alpha_n$ be a periodic orbit of $KS_n$. Then, the sequence $\{\alpha_n\}_{n=0}^\infty$ is said to be *compatible* if each $\alpha_n$ is induced by $\alpha_0$, the initial orbit of $\Delta$.

[p[3.5 cm]{} p[3.5 cm]{} p[3.5 cm]{} p[4 cm]{}]{}

![An illustration of Definitions \[def:anatomyOfKSn\](i)–(iii) in terms of $KS_0 = \Delta$ and $KS_1$. The ghost of the segment $s_{0,i}$, denoted by $g_{0,i}$, is a middle-third segment of $s_{0,i}$ and is removed from $s_{0,i}$ so that we may construct the cell $C_{1,i}$ of $KS_{1}$. Then $g_{0,i}$ is referred to as the ghost of the cell $C_{1,i}$ of $KS_{1}$.[]{data-label="fig:illustrateDefis"}](illustrateDefis1.png)

&

![An illustration of Definitions \[def:anatomyOfKSn\](i)–(iii) in terms of $KS_0 = \Delta$ and $KS_1$. The ghost of the segment $s_{0,i}$, denoted by


whereas obtuse angles of $KS_n$ constitute nonremovable singularities of that flow. Consequently, we may not be able to always determine how $\alpha$ behaves at vertices of $KS_n$. As $n$ increases, $KS_n$ grows. Therefore, we may ask whether or not an induced singular orbit $\alpha$ remains singular as $n$ increases. Because $\alpha$ can only be naturally extended at an acute angle vertex of $KS_n$, is it possible to prove that induced singular orbits always collide with acute angles? Moreover, do singular orbits which only collide with acute angles at some stage $n$ do so at every later stage $n+k$, $k\geq 1$? Even though our attention is focused on induced orbits, is it possible that there exist singular orbits of $KS_n$ that are not induced by any orbit of $\Delta$?

Ifthe behavior of $q$ over two subintervals of time $(t_0,t_1)$ and $(t_1,t_2)$. In the middle image, the corresponding periodic orbit $p_1$ would be the one induced by the initial condition $(x_{mid},\pi/3)$ and the corresponding periodic orbit $p_2$ would be induced by $((1/4,0),\pi/3)$, with the base of the generating equilateral triangle $\Delta$ lying on the $x$-axis and the lower left vertex being located at the origin.[]{data-label="fig:quasiperiodic"}](quasiperiodic1and2.png "fig:")   ![The left image depicts the quasiperiodic orbit $q$. The next two images depict the behavior of $q$ over two subintervals of time $(t_0,t_1)$ and $(t_1,t_2)$. In the middle image, the corresponding periodic orbit $p_1$ would be the one induced by the initial condition $(x_{mid},\pi/3)$ and the corresponding periodic orbit $p_2$ would be induced by $((1/4,0),\pi/3)$, with the base of the


to ask the following two questions. Firstly, if we fix $n\geq 0$ as well as a given periodic orbit $p$ of $KS_n$, is there a sequence of quasiperiodic orbits $\{q_i\}_{i=1}^\infty$ of $KS_n$ that converges to $p$, and if so, in what sense? Secondly, for a fixed quasiperiodic orbit $q$ of $KS_n$, in what ways is the induced quasiperiodic orbit of $KS_{n+1}$ qualitatively and quantitatively different from $q$? More precisely, if $q_n$ is a quasiperiodic orbit of $KS_n$, $n\geq 0$, with a fixed rational angle $a/b$ independent of $n$, and $\{q_{n+k}\}_{k=0}^\infty$ is a sequence of induced quasiperiodic orbits, is the latter sequence stable (in the sense of Definition \[def:stablequasiperiodicorbit\])?

Our experimental results thus far are indicating that we can answer all of these questions in the affirmative. If $\{a_i/b_i\}_{i=1}^\infty$ is aformula for $g(\mathcal{S}_P)$ (see, e.g., Lemma 1.2, p. 1022 of [@MaTa]) shows that $g_n = g(\mathcal{S}_{KS_n}) \to\infty$ as $n\to\infty$. Hence, it is natural to expect that the presumed limiting surface $\mathcal{S}_{KS}$ has infinite genus; see Conjecture \[conj:fractalbilliardFractalSurface\].

[^28]: For example, even if the notion of ‘inverse limit’ is suitable for formulating part (ii) or the end of part (i) of the conjecture, one would still need to specify the maps involved in the definition of the underlying inverse systems; see, e.g., [@HoYo].

[^29]: It is clearly true (and well known) that viewed as a sequence of compact subsets of $\mathbb{R}^2$, the billiard tables $KS_n$ converge in the sense of the Hausdorff metric (or, equivalently, in the Gromov–Hausdorff sense) to the Koch snowflake billiard table $KS$. Hence, the real issue concerns here


consent.
   Patrol Officer Stien, a six-year veteran of the Rockford,
Illinois, police department, testified to the following
version of events. As he approached the residence,
he heard a disturbance on the west side of the house
that he said sounded like either “glass breaking” or a “door
opening.” As Stien and Cebuhar walked Dean to the
squad car after Dean had been apprehended, Stien asked
Dean if anyone else was in the house, and Dean replied
no. Cebuhar asked Dean about the stolen rifles, and
Dean granted the officers permission to retrieve the
guns from the front closet. Stien also mentioned that the
house had a broken window and that Dean cooperated
with him, and also stated that suspect Dean had a cut
on one of his legs. Attorney Sullivan cross-examined
Stien about the nature of the sound he heardas he ap-
proached the residence and also attempted unsuccess-
fully to get Officer Stien to say that Dean refused to
consent to the search.
  Detective John Wassner testified that he heard the
breaking of glass on the west side of the residence
shortly before Dean’s apprehension. Wassner further
mentioned that, after Cebuhar had informed him that
Dean consented to the search, Wassner avoided shards of
No. 07-3627                                             5

glass in an attempt to enter the house through the broken
window on the west side of the residence.
  Dean called Joseph Taylor,


a window repairman who
said he had never met Dean. Taylor testified that on the
Saturday before the hearing he had inspected Dean’s
residence and concluded that none of the windows on
the west side had recently been broken. A friend of
Dean’s, Melvin Bradley, testified that he secured Dean’s
house after his arrest and did not observe any broken
window. Finally, Dean testified that he climbed through
a window on the west side without breaking it; after he
was caught, Dean said, one of the officers said he had
come for the guns, but Dean made no response to the
officer’s statement. On cross-examination Dean main-
tained that he injured his leg when he fell while running
from his residence and not from climbing through a
window of broken glass. He agreed that he had cooperated
with the police throughout the dayin a large amount brings about new issue of lowering the rigidity and high-temperature rigidity of the molded articles as well as the flowability of the resin compositions. Thus, it has been desired to develop a polypropylene resin composition being capable of improving the impact resistance of the molded articles with no reduction in the rigidity and high-temperature rigidity of the molded articles as well as the flowability of the resin compositions.
Accordingly, an object of the present invention is to provide a polypropylene resin composition having a well-balanced combination of the flowability of the resin composition and the rigidity, high-temperature rigidity and impact resistance of the molded article, which is suitable as a molding material for interior automotive trim parts.


= 12.26, p = 0.0005]. The test-retest showed a correlation of 0.56 (p < 0.01) between the two passations of the SHAPS. The metrological parameters of the SHAPS were discussed as well as the utility of that scale compared to the PAS.The African defender is out of favour at San Siro and his representative has played down suggestions that a move to another Serie A club this transfer window is in the pipeline

The agent of AC Milan defender Taye Taiwo has revealed that his client could leave Italy in the winter transfer window.The Nigeria international has voiced his desire for a new challenge after making just eight competitive appearances since joining the Serie A champions from Marseille in the summer.A move to Genoa as part of the deal that saw Alexander Merkel return to Milan had been tipped as a strong possibility, but Taiwo's agent has ruled out a move to the Stadio Luigi Ferraris."The player will not move to Genoa simply because they have not asked for him,"


/*
** $Id: lobject.c,v 2.22.1.1 2007/12/27 13:02:25 roberto Exp $
** Some generic functions over Lua objects
** See Copyright Notice in lua.h
*/

#include <ctype.h>
#include <stdarg.h>
#include <stdio.h>
#include <stdlib.h>
#include <string.h>

#define lobject_c
#define LUA_CORE

#include "lua.h"

#include "ldo.h"
#include "lmem.h"
#include "lobject.h"
#include "lstate.h"
#include "lstring.h"
#include "lvm.h"

const TValue luaO_nilobject_ = {{NULL}, LUA_TNIL};

/*
** converts an integer to a "floating point byte", represented as
** (eeeeexxx), where the real value is (1xxx) * 2^(eeeee - 1) if
** eeeee != 0 and (xxx) otherwise.
*/
int luaO_int2fb (unsigned int x) {
  int e = 0;  /* expoent */
  while (x >= 16) {
    x = (x+1) >> 1;
    e++;
  }
  if (x < 8) return x;
  else return ((e+1) << 3) | (cast_int(x) - 8);
}

/* converts back */
int luaO_fb2int (int x) {
  int eAlicia Menendez:

The report also cites the need to preserve older multi-family homes, better utilize public lands and change zoning rules to allow for greater building density. It also sees a role for private developers to redevelop and expand existing affordable housing. Which is exactly what is happening about six miles northwest of downtown, in a place called Liberty Square. It was built in the 1930s as one of the first segregated public housing projects for black people in the Southeast. Located in the heart of Liberty City, the area now has some of the highest rates of gun violence in Miami. These boarded up homes reflect the exodus from the community. Today, only about 200 of the original 709 units are occupied as the development is being rebuilt.


theoretical calculations. What was once touted as a test of QCD, now often plays the role of providing a description of backgrounds for searches for new types of particles. Of course, one wants these calculations to be as accurate as possible and this, in turn, requires precise knowledge of the PDFs that enter into the calculation. The error estimates on PDFs will be discussed at some length for this reason. On the other hand, there are many aspects of hadron structure that are currently not understood well, or at all, either theoretically or experimentally, and clearly identifying and delineating the limits of our knowledge in the context of global PDF fits serves a valuable purpose.

The plan of the review is as follows. Sec. 2 contains an overview of theits measurement provides important information on the subleading, higher twist contributions which parametrize long-range nonperturbative parton-parton correlations in the nucleon (see Sec. \[ssec:power\]).

### Hadron–hadron scattering. {#sssec:h-h}

As discussed in Sec. \[sec:QCD\], the PDFs are universal, the collinear singularities associated with initial parton collinear emission having been absorbed into the PDFs. Therefore, the parton distributions appearing, for example, in the expressions for DIS structure functions, are the same that describe the structure of the incoming hadrons in hadronic production. Repeating the general form given in Eq. (\[eq:xsec\]) (with $\mu_f=\mu_r \equiv \mu$), one has, for spin-unpolarized scattering, $$\begin{aligned}
\hspace*{-0.5cm}
\sigma_{A B \to C X}(p_A, p_B)
&=& \sum_{a,b} \int dx_a \, dx_b \,
    f_{a/A}(x_a, \mu)\, f_{b/B}(x_b, \mu)               \nonumber\\
& & \hspace*{0.0cm} \times


by $y_1 {\rm \ and\ } y_2$. Two-body phase constrains the momentum fractions to be $$x_a = \frac{x_T}{2} \left(e^{y_1} \, + \, e^{y_2}\right)
\ {\rm \ and\ \ }
x_b = \frac{x_T}{2} \left(e^{-y_1} \, + \, e^{-y_2}\right),
\label{eq:dijet}$$ where the dimensionless ratio $x_T = 2 p_T/\sqrt{s}$. For centrally produced dijets one sees that the parton momentum fractions are both approximately $x_T$. However, if one or both of the jets is produced at far forward or backward rapidity values, then the $x$ range can be considerably expanded towards large or small values thereby allowing a “tuning” of the probed $x$ range.

For the case of inclusive production of a jet with transverse momentum $p_T$ and rapidity $y$ there is, at LO, an integration over one of the parton momentum fractions, say $x_a$, givenWhile the valence $u_v$ and $d_v$ PDFs are fairly well constrained in the intermediate-$x$ region, at large $x$ there are significant uncertainties on the $d_v$ distribution in particular. The SU(2) nonsinglet distribution $\bar d-\bar u$ is well determined by data from the Drell-Yan reaction over the range $x \approx 0.05-0.25$, but is not constrained at higher $x$. The strange nonsinglet distribution is the most difficult to determine, requiring a combination of neutrino and antineutrino scattering data, which are subject to large experimental and nuclear uncertainties.

For the $C$-even distributions in Fig. \[fig:Spdf\], the $u+\bar u$ and $d+\bar d$ are the dominant quark distributions at large $x$, but the strange quark PDF becomes increasing more important at small $x$. Numerically, the gluon distribution dominates all other PDFs at small $x$, but


(green dotted), and NNPDF23 [@Ball:2012cx] (yellow dot-dashed) PDF parametrizations.[]{data-label="fig:dbar_ubar"}](Fig6.pdf){width="12cm"}

The earliest efforts to explain an enhancement of $\bar d$ quarks over $\bar u$ in the proton invoked the effects of Pauli blocking, which arise from the presence of different numbers of valence $u$ and $d$ quarks in the proton [@Field:1976ve]. Estimates of this effect are very difficult to quantify reliably [@Schreiber:1991tc; @Signal:1991ug], with some calculations [@Steffens:1996bc] even suggesting that it produces a small excess of $\bar u$ over $\bar d$. Alternative explanations have focused on the role of chiral symmetry breaking and the pion cloud of the nucleon [@Thomas:1983fh]. Because of the Heisenberg uncertainty principle, a component of the proton’s wave function involves its dissociation into a nucleon and a virtual pion state. The preferential coupling of a proton[@Gluck:1996ve] together with VFNS distributions, as implemented in the NuTeV analysis [@Mason:2007zz], is strictly not consistent.)

Comparison of the $\nu$ and $\bar\nu$ events found a preferred fit for the $s(x) - \bar s(x)$ distribution that peaked at $x \sim 0.05-0.1$, with the compensating negative contribution required by the sum rule $\int_0^1 dx\, (s - \bar s) = 0$ to be restricted to the unmeasured region at $x \lesssim 0.004$ [@Mason:2007zz]. For the first moment, the value obtained at $Q^2 = 16$ GeV$^2$ was $S^-\ \equiv\ \int_0^1 dx\, x (s - \bar s)
  = \left( 1.96 \pm 0.46 \pm 0.45\ {}^{+1.48}_{-1.07} \right)
    \times 10^{-3}$, where the errors are statistical, systematic, and external. The latter includes a dominant contribution from the charm semileptonic branching ratio uncertainty, as well


gluon at large $x$, since the $\bar q$ contribution is much smaller there than that of the gluon. This would also be the case for lepton pair [@Berger98:lpp] and vector boson production in $pp$ collisions, provided that one considers $p_T \gtrsim M_B/2$ in order for the parton momentum fraction to be large. The analysis in Ref. [@Carminati:2013] suggests that photon + jet data with increased statistics from the LHC may help constrain the gluon and light quark PDFs.

Another source of information on the gluon PDF is top quark pair production, for which the lowest order subprocess is $gg \to t\bar t$. In Ref. [@Czakon:2013] the constraints on the gluon PDF provided by $t \bar t$ data from the Tevatron and LHC were examined, with the results indicating that these dataplace strong constraints on the large-$x$ gluon PDF. Also of note is the analysis of ratios and double ratios of cross sections measured at different LHC energies [@Mangano:2013er]. Such ratios have reduced systematic errors and have the potential to provide strong constraints on large-$x$ PDFs.

In addition to the issues discussed above, an obstacle for the determination of the gluon distribution, and the highly correlated $\alpha_s$ values from PDF analysis, is that the calculations for the relevant processes are not available beyond NLO, with the important exceptions of the (light quark contributions to the) inclusive DIS structure functions and Drell-Yan cross sections. For example, the relative uncertainties of the JR09 gluon PDF in Fig. \[fig:gluon\] are below about 10% for $x \lesssim 0.1$, and increase as one proceeds to higher


inclusive DIS data and a $K$-factor approximation for the NLO corrections for the $pp$ data.

As for the unpolarized case in Fig. \[fig:NSpdf\], the $\Delta u^+$ distribution is the best constrained polarized PDF, mostly by measurements of the proton $g_1$ structure function over a relatively broad range of $x$. The corresponding $\Delta d^+$ distribution, which has the opposite sign, is smaller in magnitude compared with the $\Delta u^+$ with somewhat larger uncertainties, especially at larger $x$ values. The uncertainty band for the DSSV09 parametrization of $\Delta u^+$ and $\Delta d^+$ is smaller than the variation between the different PDF sets, which reflects the fact that the systematic uncertainties associated with the choice of data sets and parametrization assumptions, as well as other theoretical inputs, are currently larger than the experimentalproton and neutron $A_1$ asymmetries.

An additional feature of the helicity conservation model is that it correlates the $x \to 1$ behavior of the PDFs with the large-$Q^2$ behavior of elastic form factors [@Blankenbecler:1974tm; @Gunion:1973nm; @BrodskyLepage79], which can be measured in elastic lepton–nucleon scattering experiments at Jefferson Lab and elsewhere [@Arrington:2006zm]. This is also closely related to the notion of quark-hadron duality, which connects averages over structure functions in the resonance region at low $W$ with those extrapolated from the deep-inelastic continuum at higher $W$ (lower $x$) [@Melnitchouk:2005zr; @Melnitchouk:2001eh; @Bloom:1970xb]. Since the existing DIS data are for the most part consistent with a vanishingly small neutron asymmetry at $x \lesssim 0.5$, a very dramatic change in $A_1^n$ would be expected at larger $x$. An even more rapid transition at


data from the STAR experiment (Run 9) at RHIC [@Aggarwal:2010vc] are shown in Fig. \[fig:pol\_sea\] for zero electron rapidity, and are generally in agreement with NLO calculations using existing PDF parametrizations. Data from Run 12 at RHIC have subsequently been taken at both forward and backward rapidities [@Aschenauer:2013woa], and will provide important constraints on the antiquark polarization.

Gluon helicity {#ssec:pol_gluon}
--------------

Information on the polarized gluon distribution $\Delta g$ can be obtained in several complementary ways. Firstly, from the $Q^2$ evolution equations, the evolution of the quark singlet contribution to the $g_1$ structure function mixes with the gluon contribution, so that in principle the study of scaling violations in $g_1$ can constrain $\Delta g$. In practice, however, the $Q^2$ range and precision of the available inclusive DIS data are not sufficient to provide meaningfulwhich found a small $\Delta g/g$ at $0.05 \lesssim x \lesssim 0.35$, most of the experimental effort at measuring $\Delta g$ in $pp$ scattering has been by the PHENIX and STAR Collaborations at RHIC.

The STAR experiment measures inclusive jet production in $\vec p\, \vec p \to {\rm jet} + X$ at an invariant center of mass energy $\sqrt{s}=200$ GeV. The $A_{LL}$ data from the 2006 and 2009 runs [@Adamczyk:2012qj; @collaboration:2011fga] shown in Fig. \[fig:pol\_g\] provide the clearest evidence to date for a small but nonzero $\Delta g$. A nonzero asymmetry is also observed by STAR in preliminary data on dijet events at mid-rapidity [@Walker:2011vs], which may provide even better constraints on the shape of $\Delta g$.

The PHENIX data on inclusive neutral pion production, $\vec p\, \vec p \to \pi^0 +


X$, from 2005 to 2009 suggest a very small asymmetry up to $p_T \approx 10$ GeV [@Adare:2008aa; @Manion:2011zz]. Taken together, the inclusive RHIC data from several different channels suggest a small but non-vanishing gluon polarization in the proton. Though not as large as had been proposed in some early explanations of the small contribution of quarks to the proton spin, the precise role played by $\Delta g$ in the proton spin budget will be intriguing to understand from future measurements.

Outlook
=======

In this topical review we have presented a summary of the current knowledge of spin-averaged and (longitudinal) spin-dependent PDFs. While great progress has been made in recent years, there are still regions of Bjorken-$x$ where the PDF uncertainty bands are uncomfortably large. This is primarily due to either lack ofstructure at large $x$ in the absence of CSV effects [@Brady:2011uy; @Bjorken:1978ry; @Hobbs:2008mm; @Mantry:2010ki]. Beyond searches for CSV effects, a program of parity-violating DIS studies at the 12 GeV Jefferson Lab [@SOLID] could open up a new window on the vector $F_{1,2}^{\gamma Z}$ interference structure functions, as well as provide glimpses into the parity-odd $F_3^{\gamma Z}$ structure function.

For heavier quarks, the issue of intrinsic charm will require measuring the charm structure function at large values of $x$, which may be possible at a future Electron-Ion Collider facility [@Accardi:2012hwp]. The semi-inclusive production of prompt photons and charmed jets in $pp$ collisions at the LHC, $pp \to \gamma\, c\, X$, may produce an enhancement at large transverse momenta from intrinsic charm [@Bednyakov:2013zta].

Measurements of jet, dijet, isolated $\gamma$, and $\gamma$ + jet


functions should lead to more reliable determinations of $\Delta s$ in semi-inclusive DIS.

Finally, the polarized gluon distribution is being actively investigated in semi-inclusive deep-inelastic hadron production at COMPASS, and through double-spin asymmetries for pion and jet production in polarized $pp$ collisions at RHIC. Preliminary results from STAR on jet and dijet cross sections hint at nonzero values for $\Delta g$, which will need to be confirmed by further measurements at small $x$. Access to $\Delta g$ below $x \sim 0.05$ will be possible with future running at $\sqrt{s} = 500$ GeV and at large forward rapidity [@Aschenauer:2013woa], although reaching values down to $x \sim 10^{-4}$ will only be possible with an Electron-Ion Collider [@Accardi:2012hwp].

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separate these things. But if you listen to my other work – if you study what we teach on catalytic coaching, for example, and if you read what I’ve learned in terms of literature reviews I’ve done: traditional performance evaluations were created to protect you against your own employees and to decide about pay.

With many compensation policy systems, we normally find ourselves once a year sitting down with people, giving them a review. At the end of the review, we give them some kind of grade. And after that – shortly after that, we tell them what that translates to in terms of an increase.

And since it’s always very, very small, I mean 2%, 3%, 5%, 6% is almost always anticlimactic. But that was created this way. Andmore of a test for the ChemCam's laser."

The ChemCam system is one of 10 instruments mounted on the MSL mission's Curiosity rover—a six-wheeled mobile laboratory that will roam more than 12 miles of the planet's surface during the course of one Martian year (98 Earth weeks). The system is designed to capture as many as 14,000 observations throughout the mission.

"We are just jubilant," Wiens said. "This mission is absolutely amazing. Everything is working so well. The same applies to our instrument."

ChemCam's laser, telescope, and camera were provided by the French space agency, CNES, while the spectrometers, electronics, and software were built at Los Alamos National Laboratory, which leads the investigation. The spectrometers were developed with the aid of Ocean Optics, Incorporated, and Jet Propulsion Laboratory assisted with various


on Mars up to 7 meters (23 feet) away from the ...

With the successful launch of the Mars Science Laboratory on Saturday, Los Alamos National Laboratory researchers and scientists from the French space institute IRAP are poised to begin focusing the energy of a million light ...

Members of the Mars Science Laboratory Curiosity rover ChemCam team have received the first photos from the instrument's remote micro imager. The successful capture of ChemCam's first 10 photos sets the stage for the first ...

While Curiosity has been getting a good look around its landing spot on Mars, taking in the sights and sending back some impressive views of distant hills and Gale Crater's enormous central peak, it's also been peering very ...

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What if I told you that recentsame since then. Our mumps vaccine uses the Jeryl-Lynn strain (named after the developer’s daughter – he isolated the virus from her while she was sick with mumps). There are other strains of mumps virus also in use – the Rubini strain in Switzerland primarily, and the Urabe strain in Japan and some European countries. The Leningrad-3 strain was used in the former Soviet Union and Slovenia, and the L-Zagreb strain (a further weakened version of the Leningrad-3 strain) was used in Croatia and Slovenia. When we study how well a mumps vaccine is working, it’s important to remember that different forms of the mumps vaccine may use different strains, and it seems that some work better than others. A study showing an outbreak in a vaccinated population


of mumps were there in the pre-vaccine era?

Before 1967, when immunization for mumps started, mumps was a universal disease. That means everyone got it.

Mumps was first described by Hippocrates 2, who described in young men swelling around one or both ears, often accompanied by painful swelling of one or both testicles. During World War I, it was the leading cause of days lost from active duty in US troops deployed in France, and was the number three cause of hospitalization (only behind influenza and gonorrhea). Over the 1900s, it was identified as being caused by a virus, and by the 1950s, a vaccine had been developed in the Soviet Union, and by the 1960s, a vaccine had been developed in the United States.

With the introduction of the vaccine,am thinking of cython or a automate, but is there any way better to so this job?
thank you

A:

you can use Counter (O(n+m)) like this
from collections import Counter
lst1 = ["1","2","3"]
lst2 = ["1","3","4"]

c = Counter(lst1 + lst2)
print [i for i in c if c[i] > 1]

output
['1', '3']