proud to be CAMSC-certified. By aligning ourselves with this organization, we have taken further steps toward diversity and the economic empowerment of Aboriginal and minority companies within the promotional products industry.”

CAMSC’s mission is to deliver programs and processes that promote and facilitate procurement opportunities between major corporations in Canada and suppliers of all sizes owned and operated by Canadian Aboriginals and Minorities. For more information, visit www.camsc.ca.

Superex Now Offers Kidde Safety Products
Superex (asi/90231) is proud to announce that it now offers Kidde Safety Products in its Home Safety Products category, including the Starter Home Safety Kit (97-906XP) and the WideMouth Home Safety Kit (97-907XP). For more information, visit www.superex.com.

Bugatti-Sedona Acquires Bond Street & Stebco
Quebec City, Canada-based supplier bugatti-sedona (asi/42394) announced last month that it has acquired Bond StreetLtd., the parent company to supplier brands Bond Street and Stebco (asi/40895). Financial terms of the transaction were not released.

“This acquisition will help continue our rapid growth and market share in the United States and Canada,” said Andrew Hattem, president of bugatti-sedona. “Adding the Bond Street and Stebco icon brand will contribute in offering our customers a good, better, best approach with quality products.”

Bond Street was founded in 1917 in New York, and Stebco shortly thereafter in Chicago. The merged entity continues to be based in New York and affiliates in Montreal. “Over the years, we built an American and Canadian brand that has rivaled international players,” said Michael Schwartz, the previous owner and president of Bond Street and Stebco. “We are proud of our accomplishments and are


Q:

Should I not flag a rhetorical question posted as an answer?

I flagged this answer as not an answer. Now, I know that I was wrong because the flag was declined by a moderator. I thought that the answer was a rhetorical question (I believe it is but I could be wrong because English isn't my first language.) but didn't provide proper explanation of why the suggestion was made.
I feel that answers should be followed by a proper explanation. This answer to me looked like a comment. I have noticed in sql, lots of users don't actually provide any explanation at all but simply the queries that OP needs, which I feel is wrong but that's just me. I have done the same mistake few times but nowout because it’s not like they weren’t getting hurt. They were getting hurt, but they were just playing through it.”

Perhaps fittingly in the year Tingelhoff will be enshrined in Canton, Ohio, the Vikings have a guy who leads all active NFL centers in consecutive games started. Sullivan’s streak of 57 will take the lead if former Texans center Chris Myers (128) remains an unsigned free agent on opening day.

“Those streaks happen on their own,” Sullivan said. “Sometimes there are injuries that you just can’t play through and it’s actually better for the team if you do miss time. And better for you personally.”

The Vikings’ 22 projected starters have a combined 273 consecutive starts. Eight of them are starting over at zero. Right behind Sullivan are left tackle Matt


Two forms (I and II) of beta-N-acetyl-D-glucosaminidase from cock seminal plasma and one form (III) from spermatozoa were separated by chromatofocusing. The active enzyme forms I and II had pI values of 6.6 and 6.3, respectively, while form III had two subforms with pI values of 6.3 and 6.1, as determined by polyacrylamide gel electrofocusing. The molecular weights were 76,000 for forms I and III and 32,000 for form II. The optimum pH of enzyme forms I and III ranged from 3.6 to 4.0. In contrast, form II showed one distinct maximum at pH 3.7. The Km values obtained with p-nitrophenyl-beta-N-acetyl-D-glucosaminide as substrate were 0.35, 0.28, and 0.39 mM for forms I, II, and III, respectively. It is assumed that both cock spermatozoa and cock seminal plasma containAssociation of CETP polymorphisms with the risk of vascular dementia and white matter lesions.
Cholesteryl ester transfer protein (CETP), a component of the high density lipoprotein (HDL), plays a central role in reverse cholesterol transport. We investigated the association of two putative functional CETP polymorphisms (C-629A and I405V) with the risk of vascular dementia (VD) and tested if this association is influenced by the presence of APOE4 allele. Our study included 163 VD patients (mean age: 74.25 +/- 7.9 years) and 452 cognitively healthy probands (mean age: 70.81 +/- 7.9 years). As a biological correlate, the association of CETP gene variants with white matter lesion (WML) load was investigated. Neither the C-629A (P = 0.169) nor the I405V (P = 0.840) polymorphism was associated with VD risk in the


quality of the clubs in the Dafabet Welsh Premier League will be showcased for all to see. We would like to thank the SPFL and the Scottish FA for their vision, their invitation and their cooperation and we hope that this is the start of something quite special for all parties and especially the Welsh clubs concerned.”

Andrew Johnston, Northern Ireland Football League Managing Director, said: “The NI Football League is delighted that two of our member clubs will participate in this competition next season and I have no doubt that it will prove to be a success both on and off the pitch. It will provide a different kind of challenge for all clubs, and is a great opportunity to showcase the product on offer in the NIFL2 for more details (a copy is included in the LICENSE file that
 * accompanied this code).
 *
 * You should have received a copy of the GNU General Public License version
 * 2 along with this work; if not, write to the Free Software Foundation,
 * Inc., 51 Franklin St, Fifth Floor, Boston, MA 02110-1301 USA.
 *
 * Please contact Oracle, 500 Oracle Parkway, Redwood Shores, CA 94065 USA
 * or visit www.oracle.com if you need additional information or have any
 * questions.
 */

package sun.security.provider.certpath;

import java.io.*;
import java.security.*;
import java.security.cert.CertificateException;
import java.security.cert.CertificateParsingException;
import java.security.cert.CertPathValidatorException;
import java.security.cert.CertPathValidatorException.BasicReason;
import java.security.cert.CRLReason;
import java.security.cert.TrustAnchor;
import java.security.cert.X509Certificate;
import java.util.ArrayList;
import java.util.Arrays;
import java.util.Collections;
import java.util.Date;
import java.util.HashMap;
import java.util.List;
import java.util.Map;
import java.util.Set;
import javax.security.auth.x500.X500Principal;

import sun.security.util.HexDumpEncoder;
import sun.security.action.GetIntegerAction;
import sun.security.x509.*;
import sun.security.util.*;

/**
 * This class is used to process an OCSP response.
 * The OCSP Response is defined
 * in RFC 2560


     seq = seq.data.getDerValue();
                int version = seq.getInteger();
                if (seq.data.available() != 0) {
                    throw new IOException("Bad encoding in version " +
                        " element of OCSP response: bad format");
                }
              if (responderCert != null) {
                    certs.add(X509CertImpl.toImpl(responderCert));
                }
            } catch (CertificateException ce) {
                throw new CertPathValidatorException(
                    "Invalid issuer or trusted responder certificate", ce);
            }


MAX_CLOCK_SKEW);
        Date nowMinusSkew = new Date(now - MAX_CLOCK_SKEW);
        for (SingleResponse sr : singleResponseMap.values()) {
            if (debug != null) {
                String until = "";
                if (sr.nextUpdate != null) {
                    until = " until " + sr.nextUpdate;
                }
      name = anchor.getCA();
                pubKey = anchor.getCAPublicKey();
                certificate = anchor.getTrustedCert();
            }
        }

        /**
         * Get the certificate in this IssuerInfo if present.
         *
         * @return the {@code X509Certificate} used to create this IssuerInfo
         * object, or {@code null} if


     * would be equivalent to the certificate subject name.
         */
        X500Principal getName() {
            return name;
        }

        /**
         * Get the public key for this issuer.
         *
         * @return a {@code PublicKey} for this issuer.
         */
        PublicKey getPublicKey() {
      evolution and to better understand the evolutionary origin of beta-chymases and the Mcpt8-family, we have performed a detailed analysis of the chymase locus of four mammalian species, i.e., human, dog, mouse, and rat. As a result, we report here a second chymase-like gene in dog, Cma2, which clusters with beta-chymases in phylogenetic analyses. This finding supports a duplication of the common ancestor for alpha- and beta-chymases before the major radiation of placental mammals, and a loss of the ancestral beta-chymase gene sometime during primate evolution. Moreover, we show that in the rat, the Mcpt8-family diversified relatively recently together with sequences related to the beta-chymase Mcpt2. Eight novel genes were identified in the duplication region, four of which are predicted to be functional. Duplications of rat granzyme B- and


After the horrific school shooting in Parkland, FL, on February 14th, the "debate" about gun control has reignited in the US. Pundits on both sides of the issue are over-generalizing, taking assumptions to the extreme, and generally talking past each other. But one thing that remains constant is the left's persistent cries for "common sense" gun regulations. What constitutes "common sense" varies from person to person, but they all involve the restriction or outright ban on certain types or styles of firearms. If the War on Drugs taught us anything, it's that prohibition doesn't work, but at the same time, any number of school shootings is too many. So if bans aren't a good option, what might be? Join James Harrigan and Antony Davies as they talk aboutother transcription factors involved in inflammatory signal transduction pathways including AP-1, STAT-1 and NFAT \[[@B68-nutrients-06-04760]\].

*n*-3 PUFA can also perturb inflammatory signaling in obesity through PPARγ independent signaling mechanisms, most notably by acting as ligands for the G-protein coupled receptor 120 (GPR120) \[[@B69-nutrients-06-04760]\]. GPR120 has been shown to be partly responsible for the anti-inflammatory effects of DHA by using the adaptor β-arrestin2 to interfere with inflammatory mediator-stimulated NFκB activation in macrophages \[[@B69-nutrients-06-04760]\]. Additionally, EPA and DHA exert anti-inflammatory effects following their selective incorporation into the phospholipid fraction of cell membranes where they can act to decrease the signaling efficiency of protein complexes in lipid rafts \[[@B70-nutrients-06-04760]\], or serve as substrates for the synthesis of anti-inflammatory bioactive lipid mediators (*i.e.*, eicosanoids) \[[@B71-nutrients-06-04760],[@B72-nutrients-06-04760]\]. Taken together, *n*-3 PUFA may beneficially modulate obesity-associated


of *n*-3 PUFA on the BC phenotype \[[@B42-nutrients-06-04760],[@B43-nutrients-06-04760],[@B44-nutrients-06-04760],[@B46-nutrients-06-04760],[@B48-nutrients-06-04760],[@B49-nutrients-06-04760],[@B55-nutrients-06-04760],[@B78-nutrients-06-04760]\]. In this connection, *n*-3 PUFA are recognized for their potential application in reducing obesity-associated inflammation and consequent tumorigenic risk \[[@B45-nutrients-06-04760]\]. In brief, LC *n*-3 PUFA are incorporated into mammary AT and tumor tissue \[[@B46-nutrients-06-04760],[@B47-nutrients-06-04760]\], thereby increasing the levels of *n*-3 PUFA-derived lipid mediators at the expense of those derived from *n*-6 PUFA (*i.e.*, arachidonic acid (AA, C20:4*n*-6)-derived eicosanoids) \[[@B42-nutrients-06-04760],[@B56-nutrients-06-04760],[@B78-nutrients-06-04760]\], altering adipokine secretion \[[@B54-nutrients-06-04760]\] and interrupting tumorigenic signaling pathways \[[@B79-nutrients-06-04760]\]. These chemoprotective effects of *n*-3 PUFA result in decreased cell proliferation and increased apoptosis, ultimately resulting in reduced BC tumor incidence, growth, multiplicity, and metastasis in rodent models of BC \[[@B43-nutrients-06-04760],[@B44-nutrients-06-04760],[@B46-nutrients-06-04760],[@B48-nutrients-06-04760],[@B49-nutrients-06-04760],[@B50-nutrients-06-04760],[@B51-nutrients-06-04760],[@B52-nutrients-06-04760],[@B53-nutrients-06-04760],[@B55-nutrients-06-04760],[@B79-nutrients-06-04760]\]. Further, in a model of obese postmenopausal BC, *n*-3 PUFA supplementation reduced mammary AT inflammation and markers of inflammatory M1IL-1β and TNFα have also been shown to stimulate aromatase activity \[[@B151-nutrients-06-04760],[@B152-nutrients-06-04760],[@B153-nutrients-06-04760],[@B154-nutrients-06-04760]\]. TNFα induces aromatase expression through two mechanisms, (i) stimulating the binding of c-fos and c-jun transcription factors to activating protein-1 (AP-1) binding site; and (ii) activation of NFκB and MAPK signaling pathways \[[@B152-nutrients-06-04760],[@B153-nutrients-06-04760]\]. Obese ovariectomized rodents exhibit increased NFκB activation and inflammatory mediator production (TNF-α, IL-1β, COX-2), which is accompanied by elevated levels of aromatase expression and activity in both the mammary gland and visceral fat \[[@B120-nutrients-06-04760]\]. Collectively, these data demonstrate that inflammatory mediator signaling in the mammary tissue microenvironment is driven by autocrine/paracrine interactions that regulate critical aspects of the mammary tissue tumor phenotype including aromatase activation and local estrogen production. These inflammatory mediators can establish a positive feedback mechanism that stimulates cell proliferation and


AT macrophage accumulation, CLS formation and AT inflammation \[[@B27-nutrients-06-04760],[@B28-nutrients-06-04760]\]. We and others have shown that *n*-3 PUFA reduce inflammatory paracrine signaling between adipocytes and macrophages by decreasing NFκB activation and subsequent secretion of TNFα, MCP-1 and IL-6 \[[@B191-nutrients-06-04760],[@B192-nutrients-06-04760]\]. Moreover, independent of cellular source, *n*-3 PUFA have been shown to inhibit NFκB activation by decreasing IκB phosphorylation and activation, thereby reducing production TNFα, IL-1β and IL-6 \[[@B29-nutrients-06-04760],[@B35-nutrients-06-04760],[@B40-nutrients-06-04760],[@B41-nutrients-06-04760],[@B67-nutrients-06-04760],[@B191-nutrients-06-04760],[@B193-nutrients-06-04760],[@B194-nutrients-06-04760]\].

10. Role of Leptin
==================

Leptin exerts pleiotropic effects apart from regulation of energy expenditure and food intake, including effects on immunity, inflammation, cell differentiation and proliferation \[[@B124-nutrients-06-04760],[@B195-nutrients-06-04760]\], all of which have direct relevance to cancer. Classically, circulating leptin levels are proportional to the amount of body fat \[[@B196-nutrients-06-04760]\] and increased leptin levels are associated with increased risk of BC development and progression \[[@B197-nutrients-06-04760],[@B198-nutrients-06-04760]\]. Leptinof leptin within the mammary tissue microenvironment can ultimately promote tumorigenesis. Similar to obese women, rodents with high leptin levels are more likely to develop mammary tumors \[[@B216-nutrients-06-04760],[@B217-nutrients-06-04760]\]. Furthermore, in animal BC models leptin antagonism has produced successful outcomes. Specifically MMTV-TGF-α mice crossed with leptin deficient mice fail to develop tumors \[[@B218-nutrients-06-04760],[@B219-nutrients-06-04760]\] and treatment with a leptin antagonist decreases the growth of murine triple-negative breast tumors \[[@B220-nutrients-06-04760]\] and 4T1 mammary cancer cell growth via reducing levels of VEGF, pSTAT3 and cyclin D1 \[[@B221-nutrients-06-04760]\].

An additional role of leptin in breast carcinogenesis is to potentiate estrogen signaling, as leptin has been shown to induce aromatase expression/activity and subsequent estrogen synthesis, thereby enhancing ERα activity in BC \[[@B210-nutrients-06-04760],[@B222-nutrients-06-04760],[@B223-nutrients-06-04760]\]. Leptin levels positively correlate with ER expression and BC tumor size \[[@B203-nutrients-06-04760],[@B205-nutrients-06-04760]\]. Further,


leptin can transactivate ERα via ERK1/2 signaling \[[@B210-nutrients-06-04760]\] and enhance ERα-dependent transcription by reducing ERα ubiquitination and degradation, even in the presence of an estrogen inhibitor \[[@B223-nutrients-06-04760]\], thereby potentiating the effects of estrogen on cell proliferation. Bi-directional influences of estrogen on leptin also exist, wherein estradiol induces leptin and ObR expression, in both AT and BC cell lines \[[@B203-nutrients-06-04760],[@B224-nutrients-06-04760],[@B225-nutrients-06-04760],[@B226-nutrients-06-04760]\].

Another obesity-associated factor that can contribute to the increased local production of leptin and subsequent pro-tumorigenic effects is AT hypoxia. Leptin receptor expression can also be stimulated by tissue hypoxia \[[@B226-nutrients-06-04760]\] and, therefore, local tissue leptin expression is up-regulated by HIF-1α \[[@B227-nutrients-06-04760],[@B228-nutrients-06-04760]\]. Conversely, *n*-3 PUFA have been shown to improve the hypoxic AT microenvironment by reducing adipocyte size \[[@B27-nutrients-06-04760]\] and to decrease obesity-associated expression of HIF-1α \[[@B81-nutrients-06-04760],[@B188-nutrients-06-04760]\], thereby providing aAbout Personal Loan:

A personal loan refers to money that is borrowed from a financial institution, for personal (not professional or business) use. In opposition to larger and long-term loans, personal loans are taken into relatively short to medium terms. Generally personal loans are used to pay for one-time or short term expenses where a borrower (the person who is getting the loan) doesn't normally require disclosing the specific reason for the loan. This type of loan is used by many to resolve their current financial needs. A personal loan is taken for tenure of one to five years. Also these require lowest formalities and no collateral or security. It is a type of unsecured loan which can be availed on the basis of various criteria. Level of income,


defendant's motion for judgment on the pleadings. Plaintiff appeals.
A motion for judgment on the pleadings may be granted only when the moving party is entitled to judgment as a matter of law on the basis of the pleadings. Thayer v. Herdt, 155 Vt. 448, 456, 586 A.2d 1122, 1126 (1990). "`For the purposes of the motion all well pleaded factual allegations in the nonmovant's pleadings and all reasonable inferences that can be drawn therefrom are assumed to be true and all contravening assertions in the movant's pleadings are taken to be false.'" Id. (quoting Bressler v. Keller, 139 Vt. 401, 403, 429 A.2d 1306, 1307 (1981)). The court erroneously granted defendant's motion in favor of its affirmative defense, because there were no facts properly before the court, pledwhich is currently not fit for purpose

These people are some of society's most vulnerable, and yet they are living in homes that are not warm enough, do not contain modern facilities or are in a general state of disrepair. The chances of getting ill or having an accident are huge.

One of the saddest things I read while investigating community spirit was to learn that one million people in the UK may not have spoken to another human being in a month. And, for an estimated five million older people living alone, TV is their closest companion.

As the light dawns on a new year, so the great general election battle commences. Party leaders are out on the road, sparring over health, education and the deficit to lure undecided votes


or 3-year code signing certificate. On top of the already competitive pricing, we are offering Tucows subscribers an additional savings for each option as follows:

10% off a 1-year certificate (use Promo code: COMTUC10)

15% off a 2-year certificate (use Promo code: COMTUC15)

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What exactly is Code Signing?
Code signing is widely used to protect software that is distributed over the Internet. Code signing does not alter it; it simply appends a digital signature to the executable code itself. When customers buy software in a store, the source of that software is obvious. Customers can tell who published the software, and they can see whether the package has been opened or not. These factors enable customers to make decisions aboutwhat software to purchase and how much to "trust" those products. Customers who download digitally signed Active X controls, dynamic link libraries, .cab files or HTML content from your site can be confident that code really comes from you and hasn't been altered or corrupted since it was created and signed. Digital IDs serve as virtual "shrink-wrap" for your software: after you sign your code, if it is tampered with in any way, the digital signature will break and alert customers that the code has been altered and is not trustworthy. The solution to these issues is Microsoft's Authenticode technology coupled with Digital IDs from Comodo. Code Signing, through the use of digital signatures, enables software developers to include information about themselves and their code with their software.

What


brought in the helicopter and K-9s.

After taking Sasha for a long walk I headed over to the gym for the same core workout that I have been performing the last few Sundays with the exception of last week since it was the day after my Spartan Race:

Warm-Up

Dynamic Stretching

Main Set

Overhead Alternating Reverse Lunge w/Side Bend (8 reps per leg)

Feet-Elevated Dumbbell Alternating Chest Press (8 per arm)

Medicine Ball Transfer (12 reps)

Offset Step-up Shoulder Press (8 per leg)

Mixed-Grip Inverted Row (8 reps)

Side-to-Side Glider Plank (10 per leg)

Single-Leg Straight-Leg Deadlift and Row (8 per side)

Weighted Half-Wiper (10 per side)

1 minute rest

x3 rounds

Before starting my workout I took time to really stretch out my shoulders. It felt good to get a full stretch in.

In between sets I watched the CrossFit Games highlights againwhich helped to push me through my workout.

This workout is by far one of the hardest core workouts I have ever performed and that’s why I keep pushing myself through it each Sunday.

For the first time in a few weeks we only had to get the car washed and run to the grocery store so we were able to get back home quickly.

When we got home from the grocery store I took Sasha for a shorter walk than this morning but it was longer than it usually is.

I have been using MapMyFitness to track her walks since yesterday so that I can keep track of her walks.

As we were walking it struck me that it’s probably not your typical use case for MapMyFitness or other fitness apps. But,


How Does a Lawn Aerator Work?

By Isaiah David; Updated September 21, 2017

The Thatch Problem

As yearly growths of grass live and die, grass roots can get tangled with dead grass organic matter into a thick, matted layer called thatch. Thatch stops new grass roots from penetrating deeply into the soil and damages soil drainage as well. If the lawn gets a lot of foot traffic, it can become compacted, further weakening the grass. The grass becomes less healthy and attractive. It also becomes more vulnerable to weeds such as dandelions and thistles, as well as insect infestations.

Aeration

Aerators breaks up thatch and loosens the soil to allow the roots to spread out and water to drain properly. There are two basic types of lawn aerators: core and spike. Core aeratorssubstance
dualism and property dualism are actually really common tradeoffs in
metaphysics. A lot of times when we have two competing theories, they compete
in a specific way: one has simpler, more obvious explanations but also a
lot more shit in it, and the other one only requires like one or two things
to make it work but the explanations are banana-pants complicated.
Sometimes we call these two kinds of theories abundant and sparse
respectively.

And you can see why this might happen, right? If we could explain the entire
universe using photons, we would. Why complicate things? But we can’t explain
the entire universe just in terms of photons, so we have to add things.
So when it comes to how many things, property dualism gets to be like
"Ew, why the fuck do you have an entire separate


Headlines

Welcome to Conley's Website!

The web site of the Conley School @ SouthWood exists as an
information resource for parents, students, teachers, staff, business
partners, and community members affilliated with our school. It is the
first place to check for the latest information about academic affairs,
PTO events, Conley news, and student accomplishments. Thanks for
stopping by!

Our Vision

Conley School @ SouthWood is a place where students achieve their
maximum potential academically, socially, physically and emotionally.

Our Mission

Conley School @ SouthWood will develop a community of inquisitive,
independent, resilient learners who are Safe, Cooperative, Open-minded,
Principled, Empathetic, and able to meet the challenges of the changing
world; maximizing technology and providing engaging curriculum in a
positive learning environment.

Important Information

School Hours

School begins each day at 8:30 a.m. and continues until 2:50 p.m.

Morning supervision is available beginning at 7:45 a.m.

Afternoon supervision is availableof WeatherSTEM, an online platform that connects weather stations placed in schools around the district in order to compile all of the data the stations are collecting.
There are two separate devices on our campus, a cloud camera that records the cloud movement over our campus, and weather instruments that track things like temperature, barometric pressure, wind speed, heat index, etc.
There is a curriculum component with lesson plans that teachers can use to teach students all sorts of science, computer programming, and other STEM topics at all grade levels.
However, anyone can visit our Conley WeatherSTEM page to access the latest data!
Currently, WeatherSTEM is holding a competition to see which school can get the most Facebook "Likes" and the winner will receive small solar panels and possibly small motors to


{\rm Hom}_{\mathcal D{\rm -mod}}(P_1, D(N))\to \dots$$ By the $i=0$ case of the theorem that has already been proven, this complex is isomorphic to the complex $$0\to {\rm Hom}_{{\rm mod-}\mathcal D}(N, D(P_0))\to {\rm Hom}_{{\rm mod-}\mathcal D}(N, D(P_1))\to \dots$$ The $k$-module Ext$^i(N, D(M))$ is the $i$-th cohomology of this complex since by Lemma \[lemma\] $D(P^\bullet)$ is an injective resolution of $D(M)$. This completes the proof of Theorem \[main\].

The natural action of $\mathcal D$ on $R$ makes $R$ a left $\mathcal D$-module. Hence by Switala’s Matlis duality, $E=D(R)$ is a right $\mathcal D$-module.

\[RE\] If $N$ is a right $\mathcal D$-module, there exist $k$-linear bijections $${\rm Ext}^i_{\mathcal D{\rm  -mod}}(R,D(N))\cong {\rm Ext}^i_{{\rm mod-}\mathcal D}(N,E)$$ that are functorial in $N$.

*Proof.* This is immediate from Theorem \[main\] upon setting $M=R$.

Proof of Theorem \[maincoro\]
=============================

Throughout thisto cryptocurrencies.

However, the regulations have proven to have the opposite effect. South Koreans are trading cryptocurrencies like before, but are merely moving to foreign exchanges. The only real impact South Korea’s regulatory regime has had is pushing South Korean blockchain companies away from local exchanges. As a result, we may continue to see capital flight unless earnest steps are taken to ease the current regulatory burden.

On August 9, the South Korean exchange Prixbit closed its doors due to bankruptcy, and could very well be a bad omen of what’s to come in the country.

Do you believe the South Korean government is largely to blame for local exchanges shutting their doors? Let us know your thoughts in the comments below.

If you would like to trade Bitcoin against Tether with


Complaining about the White House’s efforts to stall the organization’s requests for death photos of the Al-Qaeda leader, Judicial Watch President Tom Fitton said, “These documents, which took nine months and a federal lawsuit to disgorge from the Obama administration, show that politically-connected filmmakers were giving extraordinary and secret access to bin Laden raid information, including the identity of a Seal Team Six leader.

“It is both ironic and hypocritical that the Obama administration stonewalled Judicial Watch’s pursuit of the bin Laden death photos, citing national security concerns, yet seemed willing to share intimate details regarding the raid to help Hollywood filmmakers release a movie ‘perfectly timed to give a home-stretch boost’ to the Obama campaign.”

Bigelow and Boal, as well as representatives for Sony Pictures, which will release theThis invention relates to a method for the preparation of oxy-diphthalic anhydrides. The products are useful chemical intermediates for the further preparation of various compounds such as the corresponding dicarboxylic acids and the various derivatives thereof, including for example, the salts, esters, acyl halides, amides, imides and the like. The oxy-diphthalic anhydrides are particularly useful as monomers in the preparation of polyimides, for example by polycondensation with a suitable diamine, such as ethylenediamine or phenylenediamine.
Various methods for the preparation of oxy-diphthalic anhydrides have been described in the chemical literature. In such method, shown to be useful in the preparation of oxy-diphthalic acids and anhydrides, involves the oxidation of tetramethyl diphenyl ethers. See Kolesnikov, G. S. et al Vysokomol. Soyed, A9, 612-18 (1967); Marvel, C. S. et al, J.


nitrite to form oxy-diphthalic anhydride.
Markezich, R. L. and Zamek, O. S. J. Org. Chem. 42, 3431 (1977) describe reaction of 4-nitrophthalimide with potassium fluoride in dimethylsulfoxide to form the corresponding oxy-diphthalimide which may be converted by hydrolysis to form the acid and ring closure to form the dianhydride.23rd Annual Pontiac Uprising

For the past 23 years, the Greater Wichita Pontiac Club has hosted Pontiac Uprising, a show-and-go event that draws Pontiacs and their owners from Kansas, Nebraska, Missouri, Oklahoma, and Texas for a weekend of sportsmanship, camaraderie, and good ol’ Pontiac fun.

Last year’s event was no exception. The festivities kicked off on Friday, October 6, 2012, with a tech seminar presented by former Pontiac dealership owner Byron Stout, and a silent auction, which netted GTOAA members Cap and Robin Proffitt a Snap-on Tools Mini Fridge.

2/12Russ Engman took home Best of Show with his resto-mod ’72 Firebird Formula.

The next day, Pontiac owners bundled up for the 40-degree temps, and headed out to Kansas International Dragway (KID) for drag racing and a Pontiac-only car show. The track opened


Q:

How can I change the directory into which SBT puts test resources?

I want the test-compile action to put the contents of src/test/resources into target/scala_2.8.1/test-classes.
The reason for this is that I'm running SBT with IntelliJ IDEA, which puts the test-classes directory on the classpath when it runs tests.
My logback-test.xml file (configuration for logback logging framework) lives in src/test/resources, and it's not being found during testing.

A:

This doesn't directly answer your question, but instead shows an the alternative that I use.
I add two new tasks: prepare and test-prepare.
lazy val prepare = task{
  None
} dependsOn (compile, copyResources) describedAs ("Compiles main, copies main resources. Use for the before-action in the idea-sbt-plugin")

lazy val testPrepare = task{
  None
} dependsOn (testCompile, copyResources, copyTestResources) describedAs ("Compiles main and test, copies all resources. Use for theEdward H. Salmon

Edward H. Salmon (born September 16, 1942) is an American politician who served in the New Jersey General Assembly from the 1st Legislative District from 1988 to 1992.

References

Category:1942 births
Category:Living people
Category:Members of the New Jersey General Assembly
Category:New Jersey Democrats


and staff of The Clubhouse at Patriot Hills and renowned Inn Credible Caterers promise to provide you and your guests with the finest quality food & service. Explore our mouth watering menus and options created for your special day.

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the original graph. Part (b) shows a breadth-first search tree of the same graph. Part (c) shows how to color the tree: starting from the root, the layers of the tree are colored alternatingly with colors 1 (dark) and 2 (light).

If there is no isolated vertex in the graph , then a weak 2-coloring determines a domatic partition: the set of the nodes with  is a dominating set, and the set of the nodes with  is another dominating set.

Applications
Historically, weak coloring served as the first non-trivial example of a graph problem that can be solved with a local algorithm (a distributed algorithm that runs in a constant number of synchronous communication rounds). More precisely, if the degree of each node is odd and bounded by adaughter, running across the street. Ms. Odendalski met Lauren in her driveway and asked her what was happening. Lauren was screaming and said that her father was trying to kill her mother. Ms. Odendalski called 911 at 10:51 p.m. Lauren told the 911 operator that she heard her mother and the appellant fighting. The appellant was hitting Mrs. Hayes on the head and chased her into Lauren's bedroom. Lauren ran into the bedroom and saw that the appellant had shot her mother in the hand. Mrs. Hayes tried to crawl under Lauren's bed to escape. Hazel Hayes, the appellant's mother, also ran to the room and tried to stop the appellant. At that point, Lauren ran out of the house and heard several more shots. During the 911


front of the appellant's black Suburban, alive, but unresponsive. Later Ms. Robinson died. Dr. Parungao testified that the cause of death was multiple gunshot wounds to the head and abdomen. Ms. Robinson was shot three times, once in the abdomen, once in the right arm, and once in the face. Ms. Robinson's white Mustang was missing.
A man named Vale Yates testified that later that same evening he stopped at a Super 8 Motel in Cleveland, Texas. He was having some trouble with the starter in his Chevy Blazer, so he left the truck running while he went inside to check in. When he returned, his Blazer was gone and parked behind where it had been was Rosalyn Robinson's white Mustang. Inside the Mustang was an overnight bag containingsec. 2(b)(1). In reviewing the sufficiency of the evidence on punishment, this Court looks at the evidence in the light most favorable to the verdict to determine whether any rational trier of fact could have believed beyond reasonable doubt *814 that the appellant would probably commit future criminal acts of violence that would constitute a continuing threat to society. See Jackson v. Virginia, 443 U.S. 307, 318-19, 99 S.Ct. 2781, 61 L.Ed.2d 560 (1979); Ladd v. State, 3 S.W.3d 547, 558 (Tex.Cr.App.1999). The circumstances of the offense alone may be sufficient to support an affirmative answer to the first special issue. Kunkle v. State, 771 S.W.2d 435, 449 (Tex.Cr.App.1986). If the circumstances of the case are sufficiently cold-blooded or calculated, then the facts alone may support a finding


addition, autopsy photographs are generally admissible unless they depict mutilation of the victim caused by the autopsy itself. Rojas v. State, 986 S.W.2d 241, 249 (Tex.Cr.App.1998). Changes rendered by the autopsy process are of minor significance if the disturbing nature of the photograph is primarily due to the injuries caused by the appellant. Santellan v. State, 939 S.W.2d 155, 173 (Tex.Cr.App.1997) (holding autopsy photographs depicting swabs in and a red stain around the victim's mouth admissible).
Exhibits 11 C, D, and E depict Mary Hayes's head and torso from three different angles. During trial Dr. Parungao testified that when he received the body it was so deformed and shattered that he had to shave the head, stitch it back together, and put paper inside of the head to expandthat he's going to testify there was a grazing wound that fractured her skull at the point.
COURT: And he opened it up to look at it closer, or that is what it looked like?
PROSECUTOR: No. He opened it up to look at it closer.
Statements made at the bench, though not heard by the jury, are still part of the record if recorded. Tex.R.App. P. 13.2(b)(3). The State's claim that this finding is unsupported by the record is incorrect.
The entry and exit wounds were relevant to the way in which the victim was killed. Without reconstruction, the jury would have seen pictures of a collapsed, bloody head. Dr. Parungao's alteration made the head less gruesome, rather than more gruesome as the appellant contends. The trial court did not abuse


morbidity, mortality, population surveillance, surveillance, vital statistics, and warming." A total of 496 article abstracts were reviewed. Where appropriate, the entire article was reviewed for more detailed information. Inclusion criteria were as follows:the article must include the words "climate change" or "global warming" in the body of its text;the article must discuss human health in a quantitative fashion using indicators;the article must make implications to suggest that climate change can affect human health or it must note the link between climate and health;the article must be relevant to the developed-world context;the article must be in English, and;the article must be retrievable electronically.

Drawing upon this literature review, we developed a list of indicators that have been used to measure climate-related health outcomes (Online Resource). We then reviewed several publicwhether arsenic is able to compromise the expression of hepatocyte nuclear factors. Also, liver histopathological examination was carried out, and several markers of hepatocyte differentiation and glucose metabolism status were determined as a measure of i-As-induced effects. Results show a consistent down-regulation of HNF1α and HNF4α under a scenario of exposure where HepG2 cells (1) gained resistance to arsenic-induced toxicity/apoptosis, (2) attained loss of tissue-specific features (as shown by the observed down-regulation of ALDOB, PEPCK and CYP1A2, triggering of the epithelial-to-mesenchymal transition program and the hypersecretion of matrix metalloproteinase-2 and 9), (3) failed to maintain balanced expression of the "stemness" genes C-MYC, OCT3/4, LIN28 and NOTCH2 and (4) showed glucose metabolism impairment. We conclude that the i-As-induced down-regulation of HNF1α and HNF4α under chronic settings may play a


is manifest, and hence, in considering a certain representation of Poincaré algebra in this framework, the representation is essentially given by translational generators. This is in consistent with the fact that the Chan-Paton factor of graviton amplitudes is described by combinations of the translational generators. Diffeomorphism invariance suggests that these generators should be furnished with generators of braid groups or Hecke-algebra-valued quantities. (For mathematical backgrounds of Hecke algebra, or Iwahori-Hecke algebra, one may refer to [@Jones:1987dy]-[@Kohno:2002bk].) A main objective of the present paper is to show that a Chan-Paton factor of a gravitational holonomy operator, which can be represented by a trace over Pincaré algebra and Iwahori-Hecke algebra, naturally leads to the Chan-Paton factor of graviton amplitudes. As in the case of gluon amplitudes, this allows us to$b_i$ of a braid group. Remember that we denote a linear representation of $b_i$ as $\rho (b_i )$. We now introduce a scaled representation $\tilde{\rho}(b_i ) = \eta \rho (b_i )$, with $\eta = q^{1/4} = \exp ( i \pi / 2 \kappa )$. It is known that the elements of $\tilde{\rho} (b_i )$ satisfy the last relation of (\[2-19\]). This can be shown by impositions of irreducibility on each of the Fock space $V_i$. (For details of this fact, one may refer to [@Kohno:2002bk].) Further, we may naturally impose a unitary condition $\tilde{b}_{i}^{-1} = \tilde{b}_{i}^{\dagger}$. Thus, the Iwahori-Hecke algebra (\[2-19\]) forms a UIR of a linear representation of braid groups, and this algebra should be encoded in the definition of a holonomy operator.

We now introduce a “comprehensive”


KZ equation $D \Psi = (d - A) \Psi = 0$. The construction is therefore similar to that of Wilson loop operators. In the present formalism, rank-$n$ differential manifolds are physically relevant for the construction. Thus, we need differential $n$-forms in terms of $A$ in order to define an appropriate holonomy operator. Further, an analog of Wilson loop should be defined on $\C$. These requirements lead to the following definition of the holonomy operator. \_[R, ]{}\^[(A)]{} (u) = \_[R, ]{} \[2-25\] where $\ga$ represents a closed path on $\C$ along which the integral is evaluated and $R$ denotes the representation of the gauge group. The color degree of freedom (or the Chan-Paton factor) can be attached to the physical operators $a_{i}^{(\pm)}$ in (\[2-21\]) as a\_[i]{}\^[()]{} = t\^[c\_i]{} a\_[i]{}\^[()c\_i]{}maximally helicity violating (MHV) graviton amplitudes can be understood as amplitudes of gauge theory (or open string theory) with an appropriate choice of a Chan-Paton factor. What to be clarified is then Chan-Paton factors of gravitons in the spinor-momenta formalism, which is a main theme of this section.

We first notice that the holonomy operator (\[2-25\]) is described by differential forms. Generally, the antisymmetrization of covariant indices and the use of exterior derivatives are required for the invariance under general coordinate transformations (or diffeomorphism). So the use of holonomy operator seems to be more natural in gravitational theories than in Yang-Mills theories. In the present formalism, a situation is not so straightforward. Namely, the bases of the “covariant” differential forms are given by the Lorentz-invariant scalar products $(u_i u_j)$


 \si_2 \si_3 \cdots \si_r \\
\end{array}%
\right)$ like the Yang-Mills case. As we will see later, a way of taking a permutation in a gravitational theory is not as simple as in the Yang-Mills case. In the present section, for simplicity of discussion, we first assume the Yang-Mills type permutation. Notice that we are going to construct a theory of gravity in a holonomy formalism. This means that a theory, and hence a graviton field, is not well-defined until a gravitational holonomy operator is constructed. Thus a full form of a comprehensive graviton field becomes transparent, once we define a gravitational holonomy operator in the next section, where the full form is obtained in (\[4-7\]). To remind us of this fact, we shall use $r$ instead of $n$ ashave not explicitly used the braid generators, however, as discussed earlier, information of braid generators is in one-to-one correspondence with permutations of the indices as long as we use an irreducible representation.

In the above expressions, the operators of $g_{i \si_i}^{(+-)}$ and $g_{i \si_i}^{(-+)}$ are naturally incorporated. These represent massless spin-zero particles with no charges. Life times of these should be the same as those of gravitons. So they are stable. We may therefore think of these spin-zero particles as a candidate for the origin of dark matter or something that couples to dark energy.

We find that $H$ in the form of (\[3-18\]) is basically given by a sum over non-vanishing products of the Chan-Paton factors of frame fields or the translational operators in tangent spaces. This is desirable


corresponds to the fact that there is only one choice of $r$ ($2 \le r \le m-3$) for $m = 5$. A structure of the diagrams is therefore uniquely determined as in Figure \[fig03\].

\[htbp\]

![Braid diagrams for $m=5$[]{data-label="fig03"}](fig03.eps){width="70mm"}

In the case of $m = 5$, the three indices to be fixed are given by $\{ 1, 4 , 5 \}$. The graviton Chan-Paton factors labeled by these indices are trivial, [*i.e.*]{}, $T^{1} = T^{4} = T^{5} = 1$. Thus nontrivial factors arise from the gravitons labeled by $\si_2 = 2$ and $\tau_{3} = 3$. From (\[3-12\]) and (\[4-3\]), we find that these are given by f ( \_2 ) & & T\^[\_2]{}  =  p\_1 p\_[\_2]{}\
( \_3 ) & & T\^[\_3]{}  =  p\_[\_3]{} p\_4 \[4-13\] Notice that these can easily be\_4 ) = T\^[\_2]{} T\^[\_3]{} T\^[\_4]{} \_[R]{} \_[\_1]{} B\_[\_2 \_3 \_4]{} \[4-17\] where we introduce notation $B_{\si_2 \si_3 \si_4}$ to indicate dependence on braid generators. An irreducible representation of the braid generators are given by the elements of Iwahori-Hecke algebra $\tilde{b}_i$ in (\[2-19\]). These elements depend on the numeric factor $\eta = \exp ( i \pi / 2 \kappa)$. Thus we expect some contributions of this factor $\eta$ in $B_{\si_2 \si_3 \si_4}$; clarification of this point is currently under investigation.

In (\[4-17\]), $\Tr_{R}$ denotes a trace over Poincaré algebra. This trace also implies a fact that we can actually use any index among $\{ 1, \si_2 , \si_3 , \si_4 \}$ as a representing index of a loop corresponding to the raising operator of the $SL (2 ,{\bf C})$


(\[2-20\])-(\[2-21\]), $A$ is defined by A &=& g \_[1 i < j n]{} A\_[ij]{} \_[ij]{} \[5-2\]\
A\_[ij]{} &=& \_[\_i]{} a\_[i]{}\^[(\_[i]{})]{} (x, ) a\_[j]{}\^[(0)]{} \[5-3\]\
\_[ij]{} & = & d (u\_i u\_j) = \[5-4\] These expressions are the same as the previous ones except that physical operators $a_{i}^{(\hat{h}_{i})}$ are now dependent on the four-dimensional chiral supercoordinate $(x, \th)$. Accordingly, the physical operators include the states of gluonic superpartners, so that the helicity index is extended from $h_i$ to $\hat{h}_{i}$ which we shall specify in a moment. In the Yang-Mills case, we consider $\N = 4$ supersymmetry. So $\th$ is written as $\th_{A}^{\al}$ $(A = 1,2; \al = 1,2,3,4)$. Projection of these Grassmann variables onto a $\cp^1$ fiber of supertwistor space is realized by \^= \_[A]{}\^ u\^A \[5-5\] In terms of these,the maximally helicity violating (MHV) amplitudes. The MHV amplitudes are the scattering amplitudes of $(n-2)$ positive-helicity gluons and $2$ negative-helicity gluons. In a momentum-space representation, the MHV tree amplitudes are expressed as \_[MHV]{}\^[(1\_+ 2\_+ r\_[-]{} s\_[-]{} n\_+ )]{} (u, ) & & \_[MHV]{}\^[(r\_[-]{} s\_[-]{})]{} (u, )\
& = & i g\^[n-2]{} (2 )\^4 \^[(4)]{} ( \_[i=1]{}\^[n]{} p\_i ) \_[MHV]{}\^[(r\_[-]{} s\_[-]{})]{} (u) \[5-9\]\
\_[MHV]{}\^[(r\_[-]{} s\_[-]{})]{} (u) &=& \_[§\_[n-1]{}]{} (t\^[c\_1]{} t\^[c\_[\_2]{}]{} t\^[c\_[\_3]{}]{} t\^[c\_[\_n]{}]{}) \[5-10\] where $u_i$ denotes the spinor momentum of the $i$-th gluon ($i=1,2, \cdots, n$). The elements $r$ and $s$ denote the numbering indices of the negative-helicity gluons. General amplitudes, the so-called non-MHV amplitudes, can be expressed in terms of the MHV amplitudes $\widehat{A}_{MHV}^{(r_{-} s_{-})} (u)$. Prescription for these expressions is called the Cachazo-Svrcek-Witten (CSW) rules. For the next-to-MHV (NMHV)


helicity configuration can be factorized by the MHV helicity configurations. Thus the helicity index is given by $h_i = (+ , -)$, rather than the supersymmetric version $\hat{h}_i = (0, \pm \frac{1}{2} , \pm )$.

Lastly, in obtaining the expression (\[5-17\]), we also use the following relations. a\_[1]{}\^[()]{} a\_[2]{}\^[(h\_2)]{} a\_[m]{}\^[(h\_m)]{} a\_[1]{}\^[(0)]{} & & a\_[2]{}\^[(h\_2)]{} a\_[m]{}\^[(h\_m)]{}\
&=& a\_[1]{}\^[()]{} a\_[2]{}\^[(h\_2)]{} a\_[m]{}\^[(h\_m)]{} \[5-20\] This relation also holds under a permutation of the numbering indices. Notice that the operators $a_{i}^{(\pm)}$ are, by construction, coupled with the logarithmic one form $\om_{ij}$. Thus the indices $(1,2, \cdots , m)$ have an antisymmetric property which we implicitly use in (\[5-20\]). This relation (\[5-20\]) has also been used in obtaining the expression (\[2-27\]).

In the following, we consider applications of the above expressions to a gravitational theory. In analogymanifest Lorentz invariance of the formalism, the Poincaré algebra is realized by translational operators in tangent spaces. A trace over Iwahori-Hecke algebra, or a braid trace, is realized by a sum over permutations of the numbering indices for gravitons. What is significant in this paper is that we clarify that the Chan-Paton factor of $\Theta_{R, \ga}^{(H)}$ is in one-to-one correspondence with a certain combinatoric factor in graviton amplitudes.

In an analysis of the Chan-Paton factor, we find that it can be characterized by three distinct loops (up to isotopy), due to an $SL(2, {\bf C})$ symmetry which is relevant to the Lorentz invariance of the logarithmic one-form $\om_{ij}$ in (\[5-24\]). The characterization can be made by a notion of ascending or descending order in the numbering indices assigned for


with increasing dose. But primary interaction between DC and LGG showed dose dependent effects. This could be due to TLR engagement and phagocytosis \[[@B25]\]. LGG is known to adhere to epithelial cells with greater ability than other*Lactobacillus* species. Such binding to DC may also increase the cellular signals triggered by direct interaction with DC. Tytgat et al. found that LGG pili S SpaCBA could interact with DC-SIGN and that blocking this interaction reduced DC cytokine production \[[@B26]\]. DC-SIGN also modulates TLR activation and it is possible that LGG pili interaction with DC-SIGN could have modulated TLR activated cytokine production. An 18 h exposure to low dose LGG produced more TNF-*α* and IL-12 than exposure to high dose LGG. It is likely that prolonged exposure led to increasing phagocytosis ofthe same right knee in practice on July 2017, while he was at the University of Miami. With injuries of this type, there are two options: repair or removal of the meniscus. Back in UI, Walker had it repaired. The timeline that has been reported by Wojnarowski, however, suggests this time he could have it removed, according to certified athletic trainer Jeff Stotts of In Street Clothes.

If that in fact is the decision, it seems like a drastic one. Removal carries a shorter recovery time, but can cause long term issues, as explained by Stotts when describing Russell Wesbrook’s options back when he was dealing with a torn meniscus:

A removal allows for a quick return to play, as the source of pain and inflammation is no longer present.


791 S.W.2d 854 (1990)
Donatus EZENWA, Respondent,
v.
DIRECTOR OF REVENUE, STATE OF MISSOURI, Appellant.
No. WD 42502.
Missouri Court of Appeals, Western District.
May 22, 1990.
William L. Webster, Atty. Gen., Jatha B. Sadowski, Sp. Asst. Atty. Gen., Jefferson City, for appellant.
Gerald L. Thompson, Kansas City, for respondent.
*855 Before SHANGLER, P.J., and CLARK and BERREY, JJ.
SHANGLER, Presiding Judge.
This is an appeal from a judgment of the circuit court in favor of the petition brought by Donatus Ezenwa, a holder of a Kansas driver's license. The petition was in two counts.
The first count was for review [presumably under § 302.311] of an order of revocation of the license to operate a motor vehicle in Missouri entered by the director of revenue. The revocation was the consequence of the refusal by Ezenwa to submit to afactEzenwa did not refuse the test on that occasion, simply does not appear in the record.
The proceeding the transcript reports resembles more an inquiry for pretrial discovery than an adjudication of contested issues on evidence. At the outset, counsel for Ezenwa explained his appearance to the court:
This is a hardship [case] ... He, on his record, has two refusals, and ourour position is that he did not get notice of the second one. If he had received notice, he would have challenged it as ... [j]ust to make him eligible for hardship driving license. I think he can only have one refusal ...
The court then inquired of the prosecutor:
Oh, okay. And you do notyou don't have any problem with that?
The prosecutor responded:
The statuteAccording to the statute, Your Honor,


this court does not have jurisdiction to grant a hardship when the Petitioner has two refusals within a five-year period. That seems to be the case on this driver's record.
Counsel for Ezenwa then informed the court that their evidence would be that Ezenwa "didn't get notice of the refusal," and also advised: "Well, I've got a problem *858 because he's [Ezenwa] not here." The court asked, nevertheless, whether there was any reason the issues of notice and that Ezenwa did not refuse to take the chemical test on June 18, 1988, could not be tried. The prosecutor replied: "Not that I know of, Your Honor."
The proceedings then reached the "evidentiary" phase:
The Court:
Have we got all the witnesses here? Counsel for Ezenwa:
Well, my client is not here now. Well,extreme ultraviolet (EUV) light. The reticle has an image printed on it. The size of the reticle is chosen for the specific system in which it is used. A reticle six inches by six inches and one-quarter inch thick can be used, for example. During lithography, a wafer, which is disposed on a wafer stage, is exposed to an image projected onto the surface of the wafer corresponding to the image printed on the reticle.
The projected image produces changes in the characteristics of a layer, for example a resist layer, deposited on the surface of the wafer. These changes correspond to the features projected onto the wafer during exposure. Subsequent to exposure, the layer can be etched to produce a patterned layer. The pattern corresponds to those features


reticle outside a SMIF pod with existing gripping devices causes the reticle to shift position significantly and to endure high surface stresses with every contact made. Furthermore, the reticle has to be gripped and released with every manipulation, in addition to those manipulations required to insert the reticle onto, or remove the reticle from, the device(s) within the lithography system that positions it within sub-100 nm accuracy. The inventor has found that this additional positioning effort dramatically increases the likelihood of sub-microscopic particle contamination. Thus, there is a need for an improved apparatus and method for holding and registering a reticle, within a vacuum environment, with minimal number of contacts made to that reticle.let it run for 20-30 minutes so that it has a chance to warm up.

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335-36. Treasure Salvors I grants the salvors title to the artifacts held by the custodian but awards only against the United States title to property outside the territorial jurisdiction. 569 F.2d at 335-36. In sum, quasi in rem jurisdiction permits a determination of rights between the parties to the litigation; the court cannot adjudicate the rights of an absent third party over whom the court enjoys no jurisdiction.
The plaintiff asserts that "this Court has, or will have during the pendency of this action, jurisdiction over any potential claimant or competing salvor by virtue of its contacts with this forum; the nature of the Plaintiff's admiralty action; the relationship of the potential claimant and/or salvor to the Plaintiff, the forum, and the cause of action; and/or the principles ofof the "shared sovereignty" of the jus gentium scuttles any application of the Titanic I rationale to a claim governed by the law of finds.
Under the law of finds, "[a] finder cannot exclude others from their attempts to obtain first possession of artifacts recovered from an abandoned wreck." Titanic III, 435 F.3d at 535. In contrast, the law of salvage grants exclusive possession to ensure that the salvor recovers the owner's property intact, and this need supports the exercise of extra-territorial jurisdiction. See Titanic III, 435 F.3d at 534-35. In other words, the law of salvage encourages the recovery of property for the benefit of the owner. A declaration granting an exclusive right to salvage the res allows the salvor to perform his duty as trustee of the


to in personam jurisdiction) unlawfully interferes with property that the plaintiff possesses, the plaintiff can employ the quasi in rem jurisdiction used in Treasure Salvors I. If the court cannot exercise in personam jurisdiction over a competing salvor in possession of the plaintiff's rightful property and the property remains outside the territorial jurisdiction of the court, a declaration of title proves useless. The court cannot force a competing salvor to return the plaintiff's rightful property without in personam jurisdiction over the competing salvor or actual control of the property.
A number of risks accompany an award of title to an uncontested wreck in international water, and these risks counsel against an expansion of admiralty in rem jurisdiction. If a competing salvor attempts to gain title to the same wreckUnrated My family has made this for years, and it was always called 'Icebox Cake' When I worked at Smith College in Northampton, Ma. they called it 'Zebra Pudding' What ever you call it, or if you add mint, it is just wonderful.... Try it, it will become a family favorite, Pam, New London, NH

Rating: Unrated we make this down in Australia but call it 'chocolate ripple cake' We use chocolate ripple biscuits which go lovely and soft like cake. Rather than use mint essence we stir broken up nestle peppermint crisps through the cream YUM!

Rating: Unrated Some grocery chains offer a 'dutch fudge' type cookie. They are not crisp, which shouldn't matter because the dessert winds up soft anyway, but they are larger and thicker, so they


Q:

Getting correct datetime

I have a file to create log entries into a text file, but the datetime will not work, I have tried setting to Utcnow but to no luck
using System;
using System.Collections.Generic;
using System.Linq;
using System.Text;
using System.IO;

namespace ParticleFramework
{
    static class Log
    {
        private static FileStream file;
        public static string dateTime = String.Format("{0:d/M/yyyy HH:mm:ss}", new DateTime());
        public static string logFile;

        public static Boolean Initialize(string f)
        {
            logFile = f;
          Senate Takes Stand for Same-Sex Couples

Some couples are losing out on Social Security and Veterans' benefits because they live in a state that doesn't recognize their union; a Senate vote, while not binding, marks an attempt to right that wrong.

The U.S. Senate wants to make sure married same-sex couples have access to all the federal benefits of marriage, even if they live in a state that doesn’t recognize their union.

In a voice vote Wednesday night, senators approved a motion calling on colleagues working out a budget deal with the House to include language assuring that “all legally married same-sex spouses have equal access to the Social Security and veterans’ benefits they have earned and receive equal treatment under the law pursuant to the Constitution,” Politico reports.

The motion, however,


func(char *p[],int r)
{
   int i;
   for(i=0;i<r;i++)
      /* At this point, p[i] is unallocated */
      scanf("%s",p[i]);
}

p[i], the thing actually storing the string, also has to be allocated. How much? Who knows, you're reading from input using scanf. So first cut is to allocate a fixed size and only read at most that size (less one because of the null character).
void func(char *p[],int r)
{
   int i;
   for( i=0; i < r; i++ ) {
       p[i] = malloc( 256 * sizeof(char) );
       scanf("%255s",p[i]);
   }
}

Never use scanf %s without a max length else the input can be larger than thememory you allocated.  Also don't use scanf, it can get you into trouble if the input doesn't match your pattern.  It's better to read the whole line with getline or fgets and then sscanf if necessary.

A memory checker is absolutely essential when coding in C. It will find these problems for you. I use valgrind.
Enter the no. of rows :5
foo
==10082== Use of uninitialised value of size 8
==10082==    at 0x1001F2121: __svfscanf_l (in /usr/lib/system/libsystem_c.dylib)
==10082==    by 0x1001EA979: scanf (in /usr/lib/system/libsystem_c.dylib)
==10082==    by 0x100000F2B: func (test.c:19)
==10082==    by 0x100000EBD: main (test.c:11)
==10082==
==10082== Invalid write of size 1
==10082==    at 0x1001F2121: __svfscanf_l (in /usr/lib/system/libsystem_c.dylib)
==10082==    by 0x1001EA979: scanf (in /usr/lib/system/libsystem_c.dylib)
==10082==    by 0x100000F2B: func (test.c:19)
==10082==


situation again in one month or six months or a year.”

This is Israel’s dilemma from the moment the low-level Gaza conflict erupted into full-scale fighting six days ago. The Palestinian death toll is nearing 100, more than half of them civilians, according to Gaza health officials. Israel has had three civilians killed by a rocket.

Invasion would push the casualty figures higher. House-to- house combat would mean more civilian deaths.

The Islamist Hamas fighters of Gaza and their junior cohorts have newly-acquired weapons such as armour-busting anti-tank guided missiles to greet the Israeli invaders, conceivably killing many more than last time.

FALLOUT

The political fallout for Prime Minister Benjamin Netanyahu at home as well as abroad could be very negative. He is running for re-election in January. The impact at the ballotof $n_1R_1$ by a factor of 2 or so [@Supplement]).

The fact of occasional piling-up of many primary CVRs, in turn, helps to explain the appearance of large-scale velocity fluctuations in the ensuing vortex tangle. In the initial random beam of primary CVRs, the fluctuations of the coarse-grained velocity on the length scales greater than $\sim n^{-1/3}$ (“quasi-classical” flow) are small; the energy spectrum is concentrated around the small length scale of order $R$. The small secondary vortex rings, observed in this work, and Kelvin waves excited by reconnections are evidence of the direct cascade of energy towards smaller length scales [@Svistunov1995; @Tsubota2000; @BarenghiRingEmission2002; @NazarenkoReconnection; @KS; @Nemirovskii2010]. However, following any of the pile-ups of many vortex rings, strong fluctuations of the coarse-grained velocity field on the “quasi-classical” length scales


radius of CVRs at collector, $x=d$, is $$R_1 = \frac{2eU}{\rho\kappa^2(\Lambda-3/2)}\label{R1}.$$ The time of flight between $x=0$ and $x=x_1$ is $$t(x) = \int_0^{x} v^{-1}dx' = \tau_1\frac{x^2}{d^2},\label{t(x)}$$ i.e. the trajectory of primary CVRs is $$x(t) = d\left(\frac{t}{\tau_1}\right)^{1/2},\label{x(t)}$$ where the time of flight from injector to collector is $$\tau_1 = \frac{4\pi e d}{\rho\kappa^3(\Lambda-1)^2}U = \frac{2\pi d}{\kappa(\Lambda-1/2)}R_1.\label{tau1}$$

The velocity field, its gradient and pulse length in $x$-space can be conveniently expressed (including the explicit time dependence along the trajectory $x(t)$): $$v\equiv \frac{{\, \mathrm{d}}x}{{\, \mathrm{d}}t} =\frac{d^2}{2\tau_1}x^{-1} = \frac{d}{2}\tau_1^{-1/2}t^{-1/2},\label{v(x)}$$ $$\nabla v = -\frac{d^2}{2\tau_1} x^{-2} = -\frac{1}{2}t^{-1},\label{nablav}$$ $$\Delta x = v\Delta t = \frac{d^2\Delta t}{2\tau_1}x^{-1} = \frac{d\Delta t}{2}\tau_1^{-1/2}t^{-1/2}.\label{Deltax}$$

Evolution of the density of CVRs
--------------------------------

The number density of primary rings in the beam $n(x,t)$, along the trajectory $x(t)$, evolves according to: $$\frac{{\, \mathrm{d}}n}{{\, \mathrm{d}}t} \equiv \frac{\partial n}{\partial t}200
        except Exception as err:
            httpcode = 404
            raise err
    except Exception as err:
        return_object = anchore_engine.common.helpers.make_response_error(err, in_httpcode=httpcode)

    return return_object, httpcode

@flask_metrics.do_not_track()
@authorizer.requires_account(with_types=INTERNAL_SERVICE_ALLOWED)
def create_object(bucket, archiveid, bodycontent):
    httpcode = 500
    try:
        account_name = ApiRequestContextProxy.namespace()
        obj_mgr = anchore_engine.subsys.object_store.manager.get_manager()

        jsonbytes = anchore_utils.ensure_bytes(json.dumps(bodycontent))
        rc = obj_mgr.put(account_name, bucket, archiveid, jsonbytes)

        my_svc =


Hi
Hello, Brother. How are you?
You were right
Emotions and all are nonsense
Now, onwards, I’ll love with my brain.
How about your college?
Did you find anyone?
Met a girl in my college, have exchanged numbers. Let’s see what happens.
Do not be a fool this time.You know what had happened before.
Yeah Bro! Now that won’t repeat.
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Hi, What are you doing?
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I was free (doing nothing). So, thought why not call you?
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Oh! No…No.
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Hey! Come on Whatsapp.
Yes! Coming.
Hello
Hello, How is your Girlfriend?
Oh! Girlfriend…. She dumped me a year back blaming me for the breakup.
Tell me about yourself.
Everything is good. I am in a relationship for 5 years but he doesn’t care about me.
Wait! Control yourself. You might fall in love with me.
Let it happen. What’sIt doesn't seem to matter who plays in goal for the New York Rangers these days. Behind arguably the best defense corps in the NHL and an opportunistic group of forwards, Henrik Lundqvist's understudies have done just fine in his absence.

The Hockey News

A source close to the New York Rangers told thn.com that the team has targeted the Rangers game March 24 against the Stanley Cup champion Los Angeles Kings for the return of Henrik Lundqvist.

But will King Henrik be able to find a place in the lineup? The Rangers are 14-2-3 with understudies Cam Talbot and Mackenzie Skapski in the lineup and have been the best team in the NHL since the calendar turned to 2015. Of course, Lundqvist will be back in the net for the


security guards,[^2] self-driving robocarts[^3], robots to help with luggages in hotels,[^4] automated hotel reception,[^5] cleaning robots,[^6] robots waiting at cafes[^7], healthcare robots [@Riek:2017:HR:3154816.3127874], and of course, autonomous vehicles.

Service robots have appeared in many places, such as Pepper[^8] in Japanese retail shops and in exhibitions as early as 2005 [@1546368], KeJia robot in a shopping mall [@doi:10.1177/1729881417703569], and a PAL REEM robot trialled in an Australian airport [@Tonkin:2018:DMU:3171221.3171270].[^9] There is no doubt that the range of use cases and applications will continue to increase. Robots might not need Internet connectivity to function, but often, many commercial service robots connect to a cloud platform and can be easily Internet-enabled, and robots may need to connect to other robots.

Rather than just speaking of robots, we will also use the more general term [*robotic things*]{} [@8525625; @7805273]with appropriate robots at the waste processing sites to sort and process the waste and so on; this robot society might work with the robot society for cleaning at certain points,

-   autonomous restaurants, with robots for cooking, taking orders, serving food, complemented by a robot society that cleans the restaurant, a robot society that grows the food (e.g., comprising farm robots and other robotic things), and a robot society responsible for transporting food from the farms to the restaurants,

-   a robot society comprising autonomous taxis, autonomous trains, autonomous wheelchairs which handle transportation needs for an area,

-   a robot society for an aged care facility, comprising not only robots to clean the building, but also to take care (to an extent) of individuals


robots along walkways, in a way that is respectful and considerate.

Think of a talking smart wall which lights up and announces advertisements as people pass near it - the wall will need to function correctly providing the right ads as programmed, but also will need to behave in ways allowed by local regulations, e.g., in terms of what form in which to make announcements (e.g., multi-lingual) and what frequency. When the wall is in operation, it should ideally be able to also lower its volume sensing conversations around it.

We might expect such behaviours also of autonomous vehicles, which need to perform their function of taking passengers to the right places, but also in a way which regulations are followed, and in a way that is safe and respectinggenerated in Prism (*P* \< 0.01) and graphically presented using Cytoscape 3.2.1. Thickness of edges (connecting lines) are proportional to *r*-values (0.4--0.99). Clusters within the dotted line were identified in patients who were also colonized with *Candida* spp.](fmicb-08-02391-g005){#F5}

Patients in clusters (1), (3), and (5) were all *Candida* negative whereas 70% of patients in clusters 2 and 4 were *Candida* positive by qPCR. Severe dysplasia (*n* = 6) was recorded in biopsies from clusters (2), (3), and (4), with three cases (50%) of severe dysplasia in cluster (3). This cluster (3) exhibited enrichments for *Leptotrichia* spp. and *Campylobacter concisus* OTU0053. Comparison of the levels of these two organisms in all patients with mild, moderate, or severe dysplasia revealed that severe dysplasia was associated with elevated levels of *Leptotrichia* spp.


db, err
}

func openOrchestratorMySQLGeneric() (db *sql.DB, fromCache bool, err error) {
	uri := fmt.Sprintf("%s:%s@tcp(%s:%d)/?timeout=%ds&readTimeout=%ds&interpolateParams=true",
		config.Config.MySQLOrchestratorUser,
		config.Config.MySQLOrchestratorPassword,
		config.Config.MySQLOrchestratorHost,
		config.Config.MySQLOrchestratorPort,
		config.Config.MySQLConnectTimeoutSeconds,
		config.Config.MySQLOrchestratorReadTimeoutSeconds,
	)
	if config.Config.MySQLOrchestratorUseMutualTLS {
		uri, _ = SetupMySQLOrchestratorTLS(uri)
	}
	return sqlutils.GetDB(uri)
}

func IsSQLite() bool {
	return config.Config.IsSQLite()
}

// OpenTopology returns the DB instance for the orchestrator backed database
func OpenOrchestrator() (db *sql.DB, err error) {
	var fromCache bool
	if IsSQLite() {
		db, fromCache, err = sqlutils.GetSQLiteDB(config.Config.SQLite3DataFile)
		if err == nil && !fromCache {
			log.Debugf("Connected to orchestrator backend: sqlite on %v", config.Config.SQLite3DataFile)
		}
		db.SetMaxOpenConns(1)
		db.SetMaxIdleConns(1)
	} else {
		if db, fromCache, err := openOrchestratorMySQLGeneric(); err != nil {
			return db, log.Errore(err)
		} else if !fromCache {
			// first time ever we talk to MySQL
			query := fmt.Sprintf("create database if not exists %s", config.Config.MySQLOrchestratorDatabase)
			if _, err := db.Exec(query); err != nil {
				return db, log.Errore(err)
			}
		}
		db, fromCache, err = sqlutils.GetDB(getMySQLURI())
		if err == nil && !fromCache {
			// do not show the password but do show what we connect to.
			safeMySQLURI := fmt.Sprintf("%s:?@tcp(%s:%d)/%s?timeout=%ds", config.Config.MySQLOrchestratorUser,
				config.Config.MySQLOrchestratorHost, config.Config.MySQLOrchestratorPort, config.Config.MySQLOrchestratorDatabase,already known to be deployed.
// This iterates both lists (to-run and already-deployed) and also verifies no contraditions.
func deployStatements(db *sql.DB, queries []string) error {
	tx, err := db.Begin()
	if err != nil {
		log.Fatale(err)
	}
	// Ugly workaround ahead.
	// Origin of this workaround is the existence of some "timestamp NOT NULL," column definitions,
	// where in NO_ZERO_IN_DATE,NO_ZERO_DATE sql_mode are invalid (since default is implicitly "0")
	// This means installation of orchestrator fails on such configured servers, and in particular on 5.7
	// where this setting is the dfault.
	// For purpose of backwards compatability, what we do is force sql_mode to be more relaxed, create the schemas
	// along with the "invalid" definition, and then go ahead and fix those definitions via following ALTER statements.
	// My bad.
	originalSqlMode := ""
	if config.Config.IsMySQL() {
		_ = tx.QueryRow(`select @@session.sql_mode`).Scan(&originalSqlMode)
		if _, err := tx.Exec(`set @@session.sql_mode=REPLACE(@@session.sql_mode,


the latest in technology, we will be by your side to help you achieve your goals or simply enjoy this beautiful game. Thanks for visiting us on-line and trust you are always welcome to visit any of our stores and share your story with us. Until then, play well.Q:

How do I Override pagination links generated by active_model_serializers

I want to override the Pagination links generated by the active_model_serializers in association with kaminari. How do I achieve this, there is no information on this page about overriding

Moreover, the links generated are in this order>> {"self", "first", "prev", "next", "last"}
I want them to be in this order instead>> {"first", "prev", "self", "next", "last"}
Below is the snippet of index method from admins controller:
  def index
    @search = Admin.search(params[:q])
    if params[:page]
      @admins = @search.result(:distinct => true).page(params[:page][:number])
    else
      @admins = @search.result(:distinct => true).page(1)
    end
    @admins_json = ActiveModel::SerializableResource.new(@admins)
    @admins_json = @admins_json.to_json(serialization_context: ActiveModelSerializers::SerializationContext.new(request))


calculated exactly. In the first method we generalize the formalism developed by Kac[@kac] for $\a=1/2$ case to arbitrary $\a$. In the second method, we use the formalism recently developed in the context of diffusion equation by Dornic and Godrèche[@dornic] using independent interval approximation (IIA). We point out however that while this latter method yields only approximate results for diffusion equation[@dornic], it gives exact results for the Markov processes that we study in this paper.

The paper is organized as follows. In section (II), we generalize Kac’s formalism for $\a=1/2$ to arbitrary $\a$ and derive an exact recursion relations satisfied by the moments of $P(m)$. In section (III), we rederive the same results by using an alternate IIA formalism. In section (IV) we use the formalism developed in sections-II andthe definition of the propagator $G$, this integral equation can then be converted to a partial differential equation, =t\^[2 -1]{} -u V(y) Q\_u(y,t) \[qproc\] with $Q_u(y,t=0)=\delta(y)$ and $V(y)=sgn(y)$.

We first make the scale transforms: z=;     a=ut;      Q\_u(y,t)= F(z,a). Substituting in Eq. \[qproc\] we get the following equation for $F$: a &=& +z +\[-a V(z)\] F\
F(z,a=0) &=& \[efeq\] where $V(z)=sgn(z)$. This equation has the following series solution: F(z,a) &=& [1]{}\_[n=0]{}\^ b\_n a\^n e\^a D\_[-n/]{}(-z) e\^[-z\^2/4]{}     z<0\
F(z,a) &=& [1]{}\_[n=0]{}\^ c\_n a\^n e\^[-a]{} D\_[-n/]{}(z) e\^[-z\^2/4]{}     z>0, \[sers\] where $D_p(z)$ are parabolic cylinder functions. The coefficients $b_n$ and $c_n$ are to be determined from the boundary conditions, namely the continuity of both $F$ and $\p F/{\p z}$ at $z=0$. The initial conditions determine $b_0=c_0=1$. Using the boundary conditions we get: \_[n=0]{}\^ b\_n a\^n e\^a D\_[-n/]{}(0) &=&


$x_O(t)=c\sqrt {t}$ where $c$ is a constant, this problem can be solved by using the techniques presented in section-II of this paper. The calculations will be similar except that the potential $V(z)=sgn (z)$ as used in Eq. \[efeq\] should be replaced by $V(z)=\theta (z-c)$. The corresponding equations can be solved as before except that now the boundary conditions are to be applied at $z=c$. We note however that the second method illustrated in section-III does not seem to be easily generalizable to solve this problem.

We conclude with one last remark. The magnetization distribution $P(m)$ is a useful quantity to study for a generic stochastic process and contain in it many useful informations regarding ergodicity etc. However as is obvious from the efforts of this paper, exact analytical calculationconsistent with ion-pairing observed at millimolar concentrations by potentiometric and spectroscopic measurements. A lower estimate for the number of water molecules that are influenced by each ion is obtained from the damped harmonic fits. Values of 19, 28 and 25 water molecules with perturbed dynamics are obtained for KFe(CN)62-, KFe(CN)63- and NaFe(CN)63- ion pairs, respectively. These values represent dynamical perturbations into a second solvation shell and are consistent with the long-range structural effects observed in recent aqueous nanodrop spectroscopy experiments. Furthermore, the spectral absorptions for hexacyanoferrates are in agreement with a wide range of solutes studied previously using the developing methodology for interpreting terahertz spectra.


hierarchy), an optional system controller, and optional interrupt controller, optional I/O or peripheral devices, etc. The memory nest is attached to a selective pairing facility via a switch or a bus. Each selectively paired processor core is includes a transactional execution facility, wherein the system is configured to enable processor rollback to a previous state and reinitialize lockstep execution in order to recover from an incorrect execution when an incorrect execution has been detected by the selective pairing facility. U.S. Patent Application Publication No. US20120210162 A1 (published Aug. 16, 2012).
U.S. Pat. No. 8,122,195 titled “Instruction for Prefetching Data and Releasing Cache Lines,” issued 2012 Feb. 21 teaches:             In general case, $$t_j {\mathrm{Env}}_\pi (D) = {\mathrm{Env}}_\pi (t_j D) \geq {\mathrm{Env}}_\pi (tD) \geq {\mathrm{Env}}_\pi (s_j D) = s_j {\mathrm{Env}}_\pi (D)$$ for any $t_j \geq t \geq s_j$ and $s_j , t_j \in {\mathbb{Q}}_{\geq0}$. Therefore we get the result by taking limit.

Let $V \subset \mathrm{Div}_{\mathbb{R}}(X_\pi)$ be a finite dimensional vector space. For any divisorial valuation $\nu$ over $X$, the map $D \mapsto \nu ({\mathrm{Env}}_\pi (D))$ is continuous on $V$.

Concave functions on a finite dimensional vector space is continuous, hence the result follows.

Let $W$ be a $X$-nef ${\mathbb{R}}$-Weil $b$-divisor over $X$. Then we have $W \leq {\mathrm{Env}}_\pi (W_\pi)$ for any birational model $\pi$ over $X$.

We fix a birational model $X_\pi$ over $X$.

[**Step1.**]{} When $W$ is a Cartier $b$-divisor determined on $\tau \geq \pi$ and $W_\tau$ is an $X$-globally generated


integral Cartier divisor, then we have $W = Z(\tau_* {\mathcal{O}}_{X_\tau} (W_\tau))$. Since $\tau_* {\mathcal{O}}_{X_\tau}(W_\tau) \subset \pi _* {\mathcal{O}}_{X_\pi}(W_\pi) $, we have $$\begin{aligned}
W = Z(\tau_* {\mathcal{O}}_{X_\tau}(W_\tau))  \leq
      Z(\pi_* {\mathcal{O}}_{X_\pi}(W_\pi) )
\leq {\mathrm{Env}}_\pi (W_\pi).\end{aligned}$$

[**Step2.**]{} Suppose $W$ is a Carteir $b$-divisor determined on $\tau \geq \pi$ and $W_\tau$ is an $X$-nef ${\mathbb{R}}$-Cartier $b$-divisor. Now there exists a sequence of $X$-very ample Cartier divisors ${A_j}$ on $X_\tau$ , a sequence of positive real numbers ${t_j}$ and finite dimensional vector space $V \subset \mathrm{Div(W_\tau)} $ such that $A_j \in V$ and $t_j A_j \to W_\tau $ as coefficient-wise. By step1, proposition 2.10, and corollary 2.11, we have $$\begin{aligned}
\nu (W) &=& \lim t_j \nu(\bar{A_j}) \\
&\leq& \lim t_j \nu({\mathrm{Env}}_{\pi} (\bar{A_j})) \\
&=& \lim \nu ({\mathrm{Env}}_\pi (t_j \bar{A_j}))\\
&=& \nu ({\mathrm{Env}}_\pi (W_\pi))\cdot W_n > -\infty$.

3.  $W_1 \cdot \ldots \cdot W_n = 0 \Rightarrow W_1 = \cdots = W_n = 0$

We have $$W_1 \cdot \ldots \cdot W_n \leq C_1 \cdot \ldots \cdot C_n$$ for all $X$-nef ${\mathbb{R}}$-Cartier $b$-divisors over $0$ such that $C_i \geq W'_i$ by the definition of intersection numbers of $b$-divisor. Thus we have the statement (1).

\(2) is clear by the definition of bounded below and (1).

If $W_i \neq 0 $ for all $i$, we can find $\epsilon > 0$ such that $W_i \leq \epsilon \cdot Z({\mathfrak{m}})$ by using corollary 3.6. Therefore we have $$W_1 \cdot \ldots \cdot W_n \leq \epsilon^n Z({\mathfrak{m}})^n < 0.$$

Properties of intersection numbers under finite morphisms
---------------------------------------------------------

In this subsection, we discuss the properties of intersection numbers under finite morphisms to consider endomorphisms.

In this subsection,


(W_1 \cdot \ldots \cdot W_n)$$

If $X$ and $Y$ have an isolated singularities, then the inequality in Proposition 3.11 is equal by [@BdFF]\[Proposition 4.16.\]. But we do not know that this inequality is equal or not in general cases.

The isolated volume and log discrepancy of non ${\mathbb{Q}}$-Gorenstein varieties
==================================================================================

In this section, we introduce log discrepancies of non ${\mathbb{Q}}$-Gorenstein varieties by using the nef envelope in place of the pullback. Here, we can consider two nef envelopes ${\mathrm{Env}}_X(K_X)$ and $-{\mathrm{Env}}_X(-K_X)$, but we use ${\mathrm{Env}}_x (K_X)$ and we state it define a good singularities with many meaning. Next, we define the isolated volume characterizing valuative log canonical singularities and we observe the properties of this invariant under finite morphisms. Finally we will prove the local statement Theorem 1.3 corresponding to the mainhave $$\frac{1}{m} \mathrm{div}(f) + {\mathrm{Env}}_X (K_X) \geq 0$$ By the condition (1), we have $K_{X_\pi} + E^\pi \geq {\mathrm{Env}}_X(K_X)_{X_\pi}$, so we have $$\frac{1}{m} \mathrm{div}_{X_\pi}(f) + K_{X_\pi} + E^\pi \geq 0$$ It means $f \in \pi_* {\mathcal{O}}_{X_\pi}(m(K_{X_\pi} + E^\pi)) $.

Proof of $\underline{(2) \Rightarrow (1)}$

By the condition (2), ${\mathrm{Env}}_X(K_X) = {\mathrm{Env}}_{X_\pi}(K_{X_\pi} + E^\pi)$. So it is enough to show ${\mathrm{Env}}_{X_\pi}(D)_\pi \leq D$ for any Weil divisor $D$ on $X_\pi$. It follows from Remark 2.14.

Next we assume $X$ has the log canonical model $X_\pi$. Now the log canonical model satisfies following conditions.

-   $K_{X_\pi} + E^\pi$ is a $X$-ample divisor.

-   $(K_{X_\pi} , E^\pi)$ is a log canonical pair.

where $E^\pi$ is the sum of the exceptional prime divisors.

Proof of $\underline{ (3) \Rightarrow (1)}$

Since $\pi$ is small, we have $$\pi_*


K_{{\mathfrak{X}}} + 1_{{\mathfrak{X}}/X} + \frac{1}{m} Z({\mathcal{O}}_X (-mK_X)) \geq 0$$ for any positive integer $m$.

Let $X_\pi$ be a log resolution of $X$. Then ${\mathrm{A}_{{\mathfrak{X}}/X}}^+ \geq 0$ if and only if $({\mathrm{A}_{{\mathfrak{X}}/X}}^+)_\pi =K_{X_\pi} + E^\pi - {\mathrm{Env}}_X(K_X)_\pi \geq 0$. In particular the non valuative log canonical set $$\mathrm{Nvlc} :=\bigcup_{\ord_E ({\mathrm{A}_{{\mathfrak{X}}/X}}^+) < 0} \mathrm{c}_X (E)$$ is a Zariski closed subset.

Let $X_\pi$ be a log resolution of $X$. Since the union of the element of $$\{ \mathrm{c}_X(E) \ | \ \mathrm{ord}_E(K_{X_\pi} + E^\pi - {\mathrm{Env}}_X(K_X)_\pi) < 0
 \mbox{, E : prime divisor on} \  X_\pi \}$$ is a closed subset of $X$, considering the complement of this set, the second assertion follows from first assertion. Thus we may assume $({\mathrm{A}_{{\mathfrak{X}}/X}}^+)_\pi \geq 0$. Let $X_\mu$ be the birational model such that $\mudetails. The purpose of this subsection is to prove the following proposition.

Let $D$ be a ${\mathbb{Q}}$-Weil divisor on $X$. The followings are equivalent

1.  $D$ is numerically ${\mathbb{Q}}$-Cartier divisor.

2.  ${\mathrm{Env}}_X(D) + {\mathrm{Env}}_X(-D) =0$

We will give a slightly different proof of [@BdFFU]. First we recall the definition of numerically ${\mathbb{Q}}$-Cartier divisors.

Let $X$ be a normal integral scheme essentially of finite type over a field and $D$ be a ${\mathbb{Q}}$-Weil divisor. $D$ is a numerically ${\mathbb{Q}}$-Cartier divisor if there exists a birational model $\pi$ and ${\mathbb{Q}}$-Weil divisor $D'$ on $X_\pi$ such that $D'$ is a $X$-numerically trivial ${\mathbb{Q}}$-Cartier divisor and $\pi_* D' = D$.

If $K_X$ is a numerically ${\mathbb{Q}}$-Cartier divisor, we say $X$ is numerically ${\mathbb{Q}}$-Gorenstein.

Let $X$ be a normal variety, $X_\pi$ be a birational model of $X$ and


Marketing and Social Media

These cookies ensure we are able to target you with content that we think are most relevant to you. These cookies also allow you to share content on social media. Deselecting these cookies may result in seeing content that is less relevant to you.of that
pressure is there. There's no danger of donations not being enough to sustain
it. The expenses are already far more than covered and it could easily stay
running in its current state forever.

~~~
city41
How do you know donations will keep up with usage? I felt like the OP was
referring to a situation where Tildes takes off and becomes large organically.

I'm currently building a site that I am considering attempting to make
possible via donations, much like Tildes. Any advice you can share? How well
have donations been working? Any gotchas? Thanks for any insights you can
share!

~~~
Deimorz
You can see the site's current expenses and donations here:
[https://tildes.net/financials](https://tildes.net/financials)

The costs to keep it running are already covered by over 10x with the current
donations, and I believe the existing servers could easily handle at least
100x the current


someone could invite me aswell. This looks really
promising.

------
Semaphor
there are several people asking for invites. pm me or reply here and I'll
invite you (Until my ten invites run out). In roughly 7h because I'm going to
sleep now.

In a recent census we realized we have very few non-tech people and women, so
please help us even the scales by reaching out if you see this ;)

~~~
Semaphor
Sadly I’m out of the edit window, so I’ll do it as a reply: If you don’t have
any contact information in your profile, I really can’t send you an invite.

------
aabbcc1241
How is it better than here?

(I like both at the moment.)

------
dredmorbius
I've been on Tildes since Early Days, same username, really like the features
and development.

And I've got a few invites. Reply and ping via email (see my HN       3367     117 (3.5)   1.52 (1.12--2.05)    1.52 (1.12--2.06)    5201     232 (4.5)   1.26 (1.06--1.51)   1.08 (0.80--1.45)
                                                                          *P*~trend~ = 0.002   *P*~trend~ = 0.004


obvious health benefits, particularly for those who are obese, our results highlight the importance of promoting injury prevention practices alongside physical activity recommendations.

This study was supported by the International Collaborative Research Grants Scheme, with joint grants from the Wellcome Trust UK (WT071587MA) and the Australian National Health and Medical Research Council (NHMRC) (268055 and 585426). SJ is supported by an Early Career Fellowship (Public Health 519796) and EB by a Senior Research Fellowship both from the NHMRC. We thank the staff at Sukhothai Thammathirat Open University (STOU) who assisted with student contact and the STOU students who are participating in the cohort study. We also thank Dr Bandit Thinkamrop and his team from Khon Kaen University for guiding us successfully through the complex data processing.

Conflicts of interest: Nonefile
  #
  # @param [String] filename  The filename of the +Procfile+ to load
  #
  def load(filename)
    @entries.replace parse(filename)
  end

  # Save a Procfile to a file
  #
  # @param [String] filename  Save the +Procfile+ to this file
  #
  def save(filename)
    File.open(filename, 'w') do |file|
      file.puts self.to_s
    end
  end

  # Get the +Procfile+ as a +String+
  #
  def to_s
    @entries.map do |name, command|
      [ name, command ].join(": ")
    end.join("\n")
  end

private

  def parse(filename)
    File.read(filename).gsub("\r\n","\n").split("\n").map do |line|
      if line =~


and debate [@Tavecchio:2010mk; @Neronov:2010bi; @Dolag:2010ni; @Broderick:2011av; @Miniati:2012ge; @Schlickeiser:2012xx]. The hint of an all pervasive magnetic field in the universe provides compelling motivation to consider particle physics processes in the early universe that can generate such a field. In turn, the detection of a cosmological magnetic field together with its power spectrum and topology (helicity) would help to identify the epoch of magnetogenesis and thereby provide information about the state of the early universe. It has been shown, for instance, that a cosmological-scale magnetic field could be generated during electroweak baryogenesis and that its helicity density is directly proportional to the baryon asymmetry of the universe [@Cornwall:1997ms; @Vachaspati:2001nb]. In this way, observations of the spectrum and helicity of cosmological magnetic fields would provide an additional handle on the originof dynamical degrees of freedom ([*e.g.*]{}, isospin, color) associated with the particle labeled $X$. There is a chemical potential for each of the Standard Model particle species: the left-handed quark doublet $Q^i = (u_L^i \, , \, d_L^i)$, the right-handed quark singlets $u_R^i$ and $d_R^i$, the left-handed lepton doublet $L^i = (\nu_L^i \, , \, e_L^i)$, the right-handed electron singlet $e_R^i$, and the scalar Higgs doublet $\Phi = (\Phi^+ \, , \, \Phi^0)$. The index $i$ indicates the generation and takes values $i = 1, 2, 3$. At all temperatures of interest, the gauge interactions are in equilibrium, and they enforce an equality of the asymmetries carried by different components of a given multiplet. For example, $\mu_{u_R^i , {\rm red}} = \mu_{u_R^i , {\rm blue}} = \mu_{u_R^i ,


[@Giovannini:1999by; @Jackiw:1999bd] and linked magnetic flux tubes [@Vachaspati:2001nb]. We use the term “hypercharge sphaleron” to refer to any ${\rm U}(1)_Y$ field configuration that interpolates between a vacuum configuration and a configuration with non-zero Chern-Simons number, which in MHD corresponds to magnetic field “helicity” (see below). Such a field configuration will source the anomaly equation for each Standard Model fermion field since they all carry hypercharge. Particle production due to the anomaly can also be understood as the emergence of filled states from the Dirac sea into the positive energy sector, just as in the case of the Abelian chiral anomaly in 3+1 dimensions [@Adam:2000gt].

The hypercharge sphaleron carries an Abelian Chern-Simons number that sources the anomaly equations, Eq. (\[eq:anomalyequations\]), and induces anomalous particle production. The corresponding particle reaction can bemagnetic field may be significantly amplified by a factor $f \sim \alpha_Y^4/ (\ecp~ \alpha_{\rm w}^2)$, which is approximately $f \sim 10^3$ for $\ecp \sim 10^{-8}$.

Based on dimensional analysis and the arguments of the preceding paragraph, we estimate the magnetic field energy density as $$\label{hrhoB}
    \rho_B \sim \frac{\alpha_Y^4}{\ecp \alpha_{\rm w}^2} \frac{h_Y}{\xi} {\, .}$$ Using Eqs. (\[eq:hY\_numerical\]) and (\[eq:xi\_initial\]) we obtain $$\label{rhoB}
    \rho_B
    \sim 10^{-5} \left(\frac{10^{-8}}{\ecp}\right) \, T^4 {\, ,}$$ where we have normalized to the value of $\ecp$ given by [Eq. (\[eq:ecp\_numerical\])]{}. This estimate shows that the backreaction of the magnetic field on the plasma can only be ignored for $\ecp \gtrsim 10^{-13}$.

Magnetic Field Evolution in a Non-Turbulent Medium {#sec:evol}
==================================================

We now turn our attention to the evolution of the magnetic field in the


as $K_p \sim \gamma_B / \gamma_D \sim \mu_0 / T$ where $\mu_0$ is the typical scale of the chiral asymmetries. For the case of leptogenesis, $\mu_0$ is fixed by the observed baryon asymmetry via [Eq. (\[lepbar\])]{}, and we obtain $k_{\rm max} \sim \mu_0 / T \sim 10^{-8}$. This corresponds to a physical length scale $l_{\rm min} = 1 / (k_{\rm max} T) \sim 10^{8} T^{-1}$. For comparison, the correlation length of the magnetic field was given by [Eq. (\[eq:xi\_initial\])]{} to be $\xi \sim 10^2 T^{-1}$. Since $\xi \ll l_{\rm min}$, the exponential amplification does not affect the modes which carry most of the power. The outcome could be different if the chiral asymmetry and/or the magnetic field correlation length were larger.

Third, the time scale for this growth is on thein which the magnetic field evolves in a non-turbulent medium, and we found that the field dissipates rapidly. The outcome is more promising if the cosmological medium is turbulent, because the associated inverse cascade provides a means of transporting power from large to small scales. As a third and final case we will suppose that turbulence is present in the cosmological medium at the epoch of magnetogenesis. We will elaborate on the assumption of turbulence at the end of this section. To be clear, however, let us remark that leptogenesis is not typically accompanied by turbulence, and this should be understood as an additional assumption. Turbulence may arise, for example, as the result of a first order phase transition. In this section, we adapt the results of analytical


anymore. This gives a range of values $10^{-13} \lesssim \ecp \lesssim 10^{-6}$, where our estimates apply. Using [Eq. (\[eq:B\_today\])]{}, we find that in the standard leptogenesis scenario accompanied by turbulence afterwards leads to the present magnetic field strength in the range $10^{-18} \lesssim B_{0}/{\rm Gauss}~ \lesssim 10^{-15}$.

The [*right-handed*]{} helicity of the magnetic field from leptogenesis can be understood heuristically by noting that $$\Delta h_A \sim \Delta h_Y \sim - \Delta n_{e_R}$$ and the equilibration process described in Sec. \[sec:equil\] gives $\Delta n_{e_R} < 0$. Since the initial electromagnetic magnetic field vanishes, we obtain $h_{A} > 0$.

In contrast to leptogenesis, it is known that magnetogenesis during electroweak baryogenesis yields a [*left-helical*]{} magnetic field [@Vachaspati:2001nb]. Measurements of the primordial magnetic field can provide an additional handle on different baryogenesis scenarios, and asmagnetic field.

As we discussed above, chiral effects play no role in the evolution of the magnetic field when the chiral asymmetry is comparable in magnitude to the observed baryon asymmetry of the universe, which is tiny. This behavior, which has been noted previously [@Joyce:1997uy], follows from the fact that the timescales of the chiral magnetic and vortical effects are inversely proportional to the magnitude of the chiral asymmetry. It is interesting to consider how our analysis would change if leptogenesis gives rise to a large initial lepton asymmetry, $\mu_0 / T = O(1)$[^7], and subsequently some unspecified physics leads to a suppression of the baryon asymmetry down to the observed level. A large injection of entropy, for example, could provided the desired suppression. In this case, the chiral


grateful to the Institute for Advanced Study, Princeton, for hospitality. AL thanks Mt. Stromlo Observatory (Australia National University) for hospitality during the completion of this work. This work was supported by the DOE at ASU.

Signs and conventions {#sec:signs}
=====================

In this Appendix we use the Minkowski metric in Cartesian coordinates: $\eta_{\mu\nu}={\rm diag}(+1, -1, -1, -1)$. The contravariant vector potential is written as $A^{\mu} = (\phi , \vca)$. The covariant vector is obtained by contraction with the 4-dimensional Minkowski metric, $A_{\mu} = \eta_{\mu\nu} A^\nu = (\phi, -{\bf A})$, and the contravariant and covariant forms of the 3-vector, $\vca$, are related by contraction with the 3-dimensional Euclidean metric $\eta^{(3)}_{ij}=\delta_{ij}$. Thus $\vca^i=\vca_i$.

The field strength tensor is defined by $F_{\mu\nu} \equiv \partial_\mu A_\nu - \partial_\nu A_\mu$ where $\partial_{0} = \partial / \partial t =
    = + \lim_{V \to \infty} \frac{1}{2V} \int dt \int_V d^3 x ~ F_{\mu\nu} {\tilde F}^{\mu\nu}~.$$

Anomaly equations {#sec:anomeqs}
=================

This appendix summarizes the chiral anomaly equations. In order to set our notation, we will first consider the chiral anomaly in massless quantum electrodynamics, and we then proceed to the Standard Model. Consider the Abelian gauge theory defined by $$\begin{aligned}
    \mathcal{L} = i \overline{\Psi} \gamma^{\mu} \left( \partial_{\mu} - i e A_{\mu} \right) \Psi - \frac{1}{4} F_{\mu \nu} F^{\mu \nu} {\, .}\end{aligned}$$ This Lagrangian is invariant under the transformations $$\begin{aligned}
    &\text{Local Gauge Transformation:} \qquad \left\{
    \begin{array}{l}
    \Psi(x) \to e^{i \theta(x)} \Psi(x) \\
    A_{\mu}(x) \to A_{\mu}(x) - \frac{1}{e} \partial_{\mu} \theta(x)
    \end{array}