Macroeconomics increasingly uses stochastic dynamic general equilibrium models to understand theoretical and policy issues. Unless very strong assumptions are made, understanding the properties of ...
More

Macroeconomics increasingly uses stochastic dynamic general equilibrium models to understand theoretical and policy issues. Unless very strong assumptions are made, understanding the properties of particular models requires solving the model using a computer. This volume brings together leading contributors in the field who explain in detail how to implement the computational techniques needed to solve dynamic economics models. It is based on lectures presented at the 7th Summer School of the European Economic Association on computational methods for the study of dynamic economies, held in 1996. A broad spread of techniques is covered, and their application to a wide range of subjects discussed. Theone‐asset version of Lucas's (1978) consumption‐based asset pricing model and the one‐sector neoclassical growth model. The discussion does not aim to exhaust the list of possible discrete state‐space methods as they are very numerous; rather it describes several examples that illustrate the basic principles involved. The main sections of the chapter describe the basic principles of numerical quadrature underlying most discrete state‐space methods, show how they can be applied in a very straightforward way to problems in which the state space consists entirely of exogenous state variables, and describe methods that can be used when there are endogenous state variables. The last section notes the several files associated with the chapter for use with MATLAB.

This chapter will critically examine today’s common ways to build equilibrium models. These specifically


sample problems regarding alternative shocks in the government and households, incomplete capital depreciation, a Real Business Cycle model with generations, and with autocorrelated shocks.Less

Competitive Business Cycles

Jean-Pascal Bénassy

Published in print: 2011-05-12

This chapter discusses the three lines of research used in assessing basic models of fluctuations in competitive markets, namely research with the use of Dynamic Stochastic General Equilibrium models, a typical Sunspot model, and a combination of Keynesian theory, the Samuelson destabilizing accelerator, and the Philips curve. It explains that the Dynamic Stochastic General Equilibrium models provide simpler solutions, as they answer simple first-order conditions of asset pricing, and address labor fluctuations. This chapter also includes sample problems regarding alternative shocks in the government and households, incomplete capital depreciation, a Real Business Cycle model with generations, and with autocorrelatedif simple, self-oriented interest rate rules are pursued by the Fed and the ECB, the losses relative to the full cooperation case will be limited to about one-tenth of steady state consumption.

This chapter examines the evolution of econometric research in business cycle analysis mainly during the 1960-90 period. It shows how the research was dominated by an assimilation of the tradition of ...
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This chapter examines the evolution of econometric research in business cycle analysis mainly during the 1960-90 period. It shows how the research was dominated by an assimilation of the tradition of NBER business cycle analysis by the CC approach, catalysed by time-series statistical methods. It also shows how the research has branched into various directions, such as the DSGE based model simulations for theory verification, device


price shock to the economy. It is found that the model economy produces reasonable posterior estimates of the structural parameters and works relatively well compared to impulse responses from the VAR with optimal prior weight from the DSGE model. A more elaborated model on government behavior is anticipated to investigate the pass-through of oil price shocks.Less

Oil Shocks in a DSGE Model for the Korean Economy

Sungbae AnKang Heedon

Published in print: 2011-03-01

This chapter describes the oil shocks using a dynamic stochastic general equilibrium (DSGE) model for the Korean economy. The Korean economy depends entirely on imports for its acquisition of crude oil, and households, entrepreneurs, and policymakers are interested in knowing to what extent the rise in oil prices affects the economy. Within an Bayesian estimation framework including DSGE-vector autoregressionspacks are expensive, but the empty Pelican case is relatively cheap. You may be able to find another front loader system, that lays nicely in a Peli.
Another interesting idea for inserts is Kickstarter

The bag listed above is not the one I use but it looks very similar, with a rubber like outer coating.

The best thing is the bags will by default contain a lot of air (they don't collapse much when closing them), so buoyancy is pretty good from the start. For my 7D with a 17-40 or 35L attached I will need next to nothing in the bag to make it float. To make sure I sometimes just keep some wrapped tissue paper in a small plastic bag inside the dry bag.

And, if possible, please do select


in conditions where one may expect big splash of water/mud/etc. - in past I used Kata E-702 but lately preferred simple no-brand clear rainsleeves (have one of them in each of my camerabags). Kata E-702 is good, but takes quite a lot of space when not used and is made from so thick plastic that using camera requires always to put hands inside the rain coat. I plan not to shoot when it's raining or water splashing - most locations won't allow to use of motor, thou I plan to buy electronic motor, so if boat is moving then I'm rowing and that won't move the boat very fast...

Now after using dry bags I'll share my experience:
Didn't work for me. Too much work to all the time openfinancial interest in the company, just a satisfied customer.

Here are a couple of how-to articles I wrote on how I use dry bags for kayaking with my camera gear. It might give you ideas that would be helpful if you are a do-it-yourself kind of guy. Maybe these ideas will give you some thoughts on useful ways to use dry bags if you choose to go that route.

Just as a sidenote, for carrying some larger dry bags or pelican cases longer distances you can always use a basic pack frame. Designed to carry heavy loads, will last forever and is pretty cheap. I use one for hauling odd loads somewhat often.


A leading progressive activist lamented Sen. Kamala Harris' departure from the 2020 race Tuesday, noting that it left only white candidates to participate in this month's Democratic debate.

"It's a sad state of affairs to have six white candidates on stage, many of whom don't necessarily speak with black women, who are the powerhouse voters -- and we're at this moment where we went from the most diverse set of candidates in the history -- certainly in my lifetime -- to an all-white stage," Aimee Allison told MSNBC's Ali Velshi on Tuesday.

Allison is the founder and president of She the People, a nonprofit dedicated to "ensur[ing] that women of color will never be taken for granted again in elections."

Her comments came after Harris, D-Calif., announced she was suspending herBELONGINGS WHILE BRIGGED

LEGAL REPRESENTATION AND TRIALS

-------------------------------

"Prisoners are permitted to seek legal representation however you are under no obligation to provide or allow this. "

(Page 4, Paragraph 1, Space Law by Nanotrasen)

- PRISONERS ARE ONLY GIVEN LEGAL REPRESENTATION WHEN THEY SEEK IT THEMSELVES

"Security personnel are under no requirement to listen to them" *IN REGARDS TO THE HEAD OF PERSONNEL AND LAWYERS

(Page 4, Paragraph 2, Space Law by Nanotrasen)

- LAWYERS AND HEAD OF PERSONNEL HAVE NO SAY IN THE LEGAL PROCESS UNLESS DIRECTED TO DO SO

"if the lawyer continuously acts as a disruptive influence Security are fully permitted to confiscate their access, remove them from the brig and bar their future access to it. "

(Page 4, Paragraph 2, Space Law by Nanotrasen)

- SECURITY (INCLUDING OFFICERS), ARE ALLOWED TO REMOVE THE


PERMITS

5. POSSESSION OF EXPLOSIVES

- TO BE IN POSSESSION OF AN EXPLOSIVE DEVICE

* EXPERIMENTAL EXPLOSIVES MUST REMAIN IN SCIENCE DEPARTMENT

6. INCITING A RIOT

- TO ATTEMPT TO STIR THE CREW INTO A RIOT

* RESTRICT RADIO AND IMPLANT TRACKING BEACON

7. SABOTAGE (SEE CAPITAL CRIMES # )

- TO HINDER THE WORK OF THE CREW OR STATION THROUGH MALICIOUS ACTIONS

* RELEASING N20, BOLTING DOORS, DISARMING POWER NETWORK, AND BARRICADES

8. THEFT

- TO STEAL RESTRICTED OR DANGEROUS ITEMS

* INCLUDES INSULATED GLOVES, SPACESUITS, JETPACKS

** CARGO BREAKING OPEN CRATES

9. MAJOR TRESPASS (SEE #10)

- BEING IN A RESTRICTED AREA WITHOUT PRIOR AUTHORIZATION

* ARMORY OR CAPTAINS QUARTERS WARRANTS 10 MINUTES AND/OR PERMANENT BRIGGING

10. BREAKING AND ENTRY OF A RESTRICTED AREA

- BREAKING AND ENTERING OF RESTRICTED AREAS

(Page 8, Paragraph 1, Space Law by Nanotrasen)

CAPITAL CRIMES

--------------

LIST OF CAPITAL CRIMES, FOLLOWING CANANALYSIS/OPINION:

Secretary of State John Kerry, echoing other policymakers in the Obama administration, blasted Israel last week in a 70-minute rant about its supposedly self-destructive policies.

Why does the world — including now the United States — single out liberal and lawful Israel but refrain from chastising truly illiberal countries?

Mr. Kerry has never sermonized for so long about his plan to solve the Syrian crisis that has led to some 500,000 deaths or the vast migrant crisis that has nearly wrecked the European Union.

No one in this administration has shown as much anger about the many thousands who have been killed and jailed in the Castro brothers’ Cuba, much less about the current Stone Age conditions in Venezuela or the nightmarish government of President Rodrigo Duterte in the Philippines, an


No.
                                                        71D05-1302-CT-21

Brown, Judge.

Court of Appeals of Indiana | Opinion 71A03-1608-CT-1927 | November 17, 2017                           Page 1 of 15
[1]   Marvin Podemski appeals the trial court’s entry of summary judgment in favor

      of Praxair, Inc. (“Praxair”) and Antibus Scales & Systems, Inc. matter of law. Manley v. Sherer, 992 N.E.2d 670, 673 (Ind. 2013). Summary

       judgment is improper if the moving party fails to carry its burden, but if it

       succeeds, then the nonmoving party must come forward with evidence

       establishing the existence of a genuine issue of material fact. Id. We construe

       all factual inferences in favor of the nonmoving party and resolve all doubts as

       to the existence of a material issue against the moving party. Id. In the
       Court of Appeals of Indiana | Opinion 71A03-1608-CT-1927 | November 17, 2017


     command.CommandText = "SELECT * FROM Files";
        conn.Open();

        MySqlDataReader reader = command.ExecuteReader();
        while (reader.Read())
        {
            //How to output the rows ????
        }
    }
    catch (Exception ex)
    {
        Console.WriteLine(ex.Message);
    }

    return null; // return the list
}

A:

Making some assumptions about your File Table, this is how you get the data
public IEnumerable<File> Get()
{
    List<File> list =season, teams were allowed to schedule twelve regular season games instead of eleven leading to additional revenues for all teams and allowing players the enhanced opportunity to break various statistical records.

Rules changes
The NCAA Rules Committee adopted the following rules changes for the 2002 season:
 The penalty for violating the so-called "Halo Rule" (two yard restricted area around the punt/kick receiver) without making contact with the receiver is increased from five yards to 10 yards.
 Flagrant personal fouls committed during possession by the defense in overtime will be carried over to the next extra period.  Previously, those fouls were disregarded but the player committing the foul was ejected from the game.
 All players are required to wear facemasks of the same color.
 Penalties committed during a


LGK-974, an effective and specific PORCN inhibitor that can prevent the formation of a proper folding of the Wnt protein in the endoplasmic reticulum. We found that HepG2 cells became more sensitive to radiation with increasing LGK-974 concentrations. Upon 2 Gy or 4 Gy irradiation, the cells treated with LGK-974 more frequently underwent apoptosis and grew less rapidly. PCR and western blot results showed that inhibiting the secretion of Wnt3A blocked the Wnt signaling pathway and prevented Nrf2 signaling. Notably, the Wnt inhibitor may serve as a radiosensitizing drug.continue to bring you the latest news, reviews, and competitions. Follow us on Facebook and Twitter to keep up with the latest technology. Share your favourite articles, chat with the team and more. Also check out eTeknix YouTube, where you'll find our latest video reviews, event coverage and features in 4K!

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bit definitions.
 */
enum {
	FRC_ECC_ERR_VW = (1 << 12),
	FRC_ECC_ERR_VB = (1 << 13),
	FRC_ECC_ERR_NI = (1 << 14),
	FRC_ECC_ERR_NO = (1 << 15),
	FRC_ECC_PFE_SHIFT = 16,
	FRC_ECC_ERR_DO = (1 << 18),
	FRC_ECC_P14 = (1 << 19),
};

/*
 *  Error Status Register (ERR_STS) bit definitions.
 */
enum {
	ERR_STS_NOF = (1 << 0),
	ERR_STS_NIF = (1 << 1),
	ERR_STS_DRP = (1 << 2),
	ERR_STS_XGP = (1 << 3),
	ERR_STS_FOU = (1 << 4),
	ERR_STS_FOC = (1 << 5),
	ERR_STS_FOF = (1 << 6),
	ERR_STS_FIU = (1 << 7),
	ERR_STS_FIC = (1 << 8),
	ERR_STS_FIF = (1 << 9),
	ERR_STS_MOF = (1 << 10),
	ERR_STS_TA = (1 << 11),
	ERR_STS_MA = (1 << 12),
	ERR_STS_MPE = (1 << 13),
	ERR_STS_SCE = (1 << 14),
	ERR_STS_STE = (1 << 15),
	ERR_STS_FOW = (1 << 16),
	ERR_STS_UE = (1 << 17),
	ERR_STS_MCH = (1 << 26),
	ERR_STS_LOC_SHIFT = 27,
};

/*
 *  RAM Debug Address Register (RAM_DBG_ADDR) bit definitions.
 */
enum29),
};

/*
 *  Stop CQ Processing Register (CQ_STOP) bit definitions.
 */
enum {
	CQ_STOP_QUEUE_MASK = (0x007f0000),
	CQ_STOP_TYPE_MASK = (0x03000000),
	CQ_STOP_TYPE_START = 0x00000100,
	CQ_STOP_TYPE_STOP = 0x00000200,
	CQ_STOP_TYPE_READ = 0x00000300,
	CQ_STOP_EN = (1 << 15),
};

/*
 *  MAC Protocol Address Index Register (MAC_ADDR_IDX) bit definitions.
 */
enum {
	MAC_ADDR_IDX_SHIFT = 4,
	MAC_ADDR_TYPE_SHIFT = 16,
	MAC_ADDR_TYPE_COUNT = 10,
	MAC_ADDR_TYPE_MASK = 0x000f0000,
	MAC_ADDR_TYPE_CAM_MAC = 0x00000000,
	MAC_ADDR_TYPE_MULTI_MAC = 0x00010000,
	MAC_ADDR_TYPE_VLAN = 0x00020000,
	MAC_ADDR_TYPE_MULTI_FLTR = 0x00030000,
	MAC_ADDR_TYPE_FC_MAC = 0x00040000,
	MAC_ADDR_TYPE_MGMT_MAC = 0x00050000,
	MAC_ADDR_TYPE_MGMT_VLAN = 0x00060000,
	MAC_ADDR_TYPE_MGMT_V4 = 0x00070000,
	MAC_ADDR_TYPE_MGMT_V6 = 0x00080000,
	MAC_ADDR_TYPE_MGMT_TU_DP = 0x00090000,
	MAC_ADDR_ADR = (1 << 25),
	MAC_ADDR_RS = (1 << 26),
	MAC_ADDR_E = (1 << 27),
	MAC_ADDR_MR = (1 << 30),
	MAC_ADDR_MW = (1 << 31),
	MAX_MULTICAST_ENTRIES = 32,

	/* Entry count and words per entry
	 * for each address type in the filter.
	 */
	MAC_ADDR_MAX_CAM_ENTRIES = 512,
	MAC_ADDR_MAX_CAM_WCOUNT = 3,
	MAC_ADDR_MAX_MULTICAST_ENTRIES = 32,
	MAC_ADDR_MAX_MULTICAST_WCOUNT = 2,
	MAC_ADDR_MAX_VLAN_ENTRIES = 4096,
	MAC_ADDR_MAX_VLAN_WCOUNT = 1,
	MAC_ADDR_MAX_MCAST_FLTR_ENTRIES = 4096,
	MAC_ADDR_MAX_MCAST_FLTR_WCOUNT = 1,
	MAC_ADDR_MAX_FC_MAC_ENTRIES = 4,
	MAC_ADDR_MAX_FC_MAC_WCOUNT = 2,
	MAC_ADDR_MAX_MGMT_MAC_ENTRIES = 8,
	MAC_ADDR_MAX_MGMT_MAC_WCOUNT = 2,
	MAC_ADDR_MAX_MGMT_VLAN_ENTRIES =


OB_MAC_IOCB_LEN_MASK 0x3ffff
	__le16 reserved2;
	u32 tid;
	u32 txq_idx;
	__le32 reserved3;
	__le16 vlan_tci;
	__le16 reserved4;
	struct tx_buf_desc tbd[TX_DESC_PER_IOCB];
} __packed;

struct ob_mac_iocb_rsp {
	u8 opcode;		/* */
	u8 flags1;		/* */
#define OB_MAC_IOCB_RSP_OI	0x01	/* */
#define OB_MAC_IOCB_RSP_I	0x02	/* */
#define OB_MAC_IOCB_RSP_E	0x08	/* */
#define OB_MAC_IOCB_RSP_S	0x10	/* too Short */
#define OB_MAC_IOCB_RSP_L	0x20	/* too Large */
#define OB_MAC_IOCB_RSP_P	0x40	/* Padded */
	u8 flags2;		/* */
	u8 flags3;		/* */
#define OB_MAC_IOCB_RSP_B	0x80	/* */
	u32 tid;
	u32 txq_idx;
	__le32 reserved[13];
} __packed;

struct ob_mac_tso_iocb_req {
	u8 opcode;
	u8 flags1;
#define OB_MAC_TSO_IOCB_OI	0x01
#define OB_MAC_TSO_IOCB_I	0x02
#define OB_MAC_TSO_IOCB_D	0x08
#define OB_MAC_TSO_IOCB_IP4	0x40
#define OB_MAC_TSO_IOCB_IP6	0x80
	u8 flags2;
#define OB_MAC_TSO_IOCB_LSO	0x20
#define OB_MAC_TSO_IOCB_UC	0x40
#define OB_MAC_TSO_IOCB_TC	0x80
	u8 flags3;
#define OB_MAC_TSO_IOCB_IC	0x01
#define OB_MAC_TSO_IOCB_DFP	0x02
#define OB_MAC_TSO_IOCB_V	0x04
	__le32 reserved1[2];
	__le32 frame_len;
	u32 tid;
	u32 txq_idx;
	__le16 total_hdrs_len;
	__le16 net_trans_offset;
#define OB_MAC_TRANSPORT_HDR_SHIFT 6
	__le16 vlan_tci;
	__le16 mss;
	struct tx_buf_desc tbd[TX_DESC_PER_IOCB];
} __packed;

struct ob_mac_tso_iocb_rsp {
	u8 opcode;
	u8 flags1;
#define OB_MAC_TSO_IOCB_RSP_OI	0x01
#define OB_MAC_TSO_IOCB_RSP_I	0x02
#define OB_MAC_TSO_IOCB_RSP_E	0x08
#define OB_MAC_TSO_IOCB_RSP_S	0x10
#define OB_MAC_TSO_IOCB_RSP_L	0x20
#define OB_MAC_TSO_IOCB_RSP_P	0x40
	u8 flags2;		/* */
	u8 flags3;		/* */
#define OB_MAC_TSO_IOCB_RSP_B	0x8000
	u32 tid;
	u32 txq_idx;
	__le32 reserved2[13];
} __packed;

struct ib_mac_iocb_rsp {
	u8 opcode;		/* 0x20 */
	u8 flags1;
#define IB_MAC_IOCB_RSP_OI	0x01	/* Overide intr delay */
#define IB_MAC_IOCB_RSP_I	0x02	/* Disble Intr Generation */
#define IB_MAC_CSUM_ERR_MASK 0x1c	/* A mask to use for csum errs */
#define IB_MAC_IOCB_RSP_TE	0x04	/* Checksum error */
#define IB_MAC_IOCB_RSP_NU	0x08	/* No checksum rcvd */
#defineserdes_xfi_hss_pcs[XG_SERDES_XFI_HSS_PCS_COUNT];

	/* segment 27 */
	struct mpi_coredump_segment_header xfi_hss_tx_hdr;
	u32 serdes_xfi_hss_tx[XG_SERDES_XFI_HSS_TX_COUNT];

	/* segment 28 */
	struct mpi_coredump_segment_header xfi_hss_rx_hdr;
	u32 serdes_xfi_hss_rx[XG_SERDES_XFI_HSS_RX_COUNT];

	/* segment 29 */
	struct mpi_coredump_segment_header xfi_hss_pll_hdr;
	u32 serdes_xfi_hss_pll[XG_SERDES_XFI_HSS_PLL_COUNT];

	/* segment 30 */
	struct mpi_coredump_segment_header misc_nic_seg_hdr;
	struct ql_nic_misc misc_nic_info;

	/* segment 31 */
	/* one interrupt state for each CQ */
	struct mpi_coredump_segment_header intr_states_seg_hdr;
	u32 intr_states[MAX_RX_RINGS];

	/* segment 32 */
	/* 3 cam words each for 16 unicast,
	 * 2 cam words for each of 32 multicast.
	 */
	struct mpi_coredump_segment_header cam_entries_seg_hdr;
	u32 cam_entries[(16 * 3) + (32 * 3)];

	/* segment 33 */
	struct mpi_coredump_segment_header nic_routing_words_seg_hdr;
	u32 nic_routing_words[16];
	/* segment 34 */
	struct mpi_coredump_segment_header ets_seg_hdr;
	u32 ets[ETS_REGS_DUMP_WORD_COUNT];

	/* segment 35 */
	struct mpi_coredump_segment_header probe_dump_seg_hdr;
	u32 probe_dump[PRB_MX_DUMP_TOT_COUNT];

	/* segment 36 */
	struct mpi_coredump_segment_header routing_reg_seg_hdr;
	u32 routing_regs[RT_IDX_DUMP_TOT_WORDS];

	/* segment 37 */
	struct mpi_coredump_segment_header mac_prot_reg_seg_hdr;
	u32 mac_prot_regs[MAC_ADDR_DUMP_TOT_WORDS];

	/* segment 38 */
	struct mpi_coredump_segment_header xaui2_an_hdr;
	u32 serdes2_xaui_an[XG_SERDES_XAUI_AN_COUNT];

	/* segment 39 */
	struct mpi_coredump_segment_header xaui2_hss_pcs_hdr;
	u32 serdes2_xaui_hss_pcs[XG_SERDES_XAUI_HSS_PCS_COUNT];

	/* segment 40 */
	struct mpi_coredump_segment_header xfi2_an_hdr;
	u32 serdes2_xfi_an[XG_SERDES_XFI_AN_COUNT];

	/* segment 41 */
	struct mpi_coredump_segment_header xfi2_train_hdr;
	u32 serdes2_xfi_train[XG_SERDES_XFI_TRAIN_COUNT];

	/* segment 42 */
	struct mpi_coredump_segment_header xfi2_hss_pcs_hdr;
	u32 serdes2_xfi_hss_pcs[XG_SERDES_XFI_HSS_PCS_COUNT];

	/*


                uint32_t initial_size,
                    uint64_t bo_flags)
{
   VkResult result;

   pool->device = device;
   pool->bo_flags = bo_flags;
   pool->start_address = gen_canonical_address(start_address);

   anv_bo_init(&pool->bo, 0, 0);

   pool->fd = memfd_create("block pool", MFD_CLOEXEC);
   if (pool->fd == -1)
      return vk_error(VK_ERROR_INITIALIZATION_FAILED);

   /* Just make it 2GB up-front.  The Linux kernel won't actually back it
    * with pages until we either map and fault on one of them or we use
    * userptr and send a chunk of32-bit addresses.  We could also pin the
    * BO to some particular location of our choosing, but that's significantly
    * more work than just not setting a flag.  So, we explicitly DO NOT set
    * the EXEC_OBJECT_SUPPORTS_48B_ADDRESS flag and the kernel does all of the
    * hard work for us.
    */
   anv_bo_init(&pool->bo, gem_handle, size);
   if (pool->bo_flags & EXEC_OBJECT_PINNED) {
      pool->bo.offset = pool->start_address + BLOCK_POOL_MEMFD_CENTER -
         center_bo_offset;
   }
   pool->bo.flags = pool->bo_flags;
   pool->bo.map = map;

   return VK_SUCCESS;
}

/** Grows and re-centers the block pool.
 *
 * We grow the


       *       two-level split.  If it's bigger than some fixed block_size,
          *       we split it into block_size sized chunks and return all but
          *       one of them.  Then we split what remains into
          *       state.alloc_size sized chunks and return all but one.
          *
          * We choose option (3).
          * all but the first block of the chunk to the block bucket.
             */
            const uint32_t block_bucket =
               anv_state_pool_get_bucket(pool->block_size);
            anv_free_list_push(&pool->buckets[block_bucket].free_list,
                               pool->block_pool.map,


    struct bo_pool_bo_link link_copy = VG_NOACCESS_READ(link);

         anv_gem_munmap(link_copy.bo.map, link_copy.bo.size);
         anv_vma_free(pool->device, &link_copy.bo);
         anv_gem_close(pool->device, link_copy.bo.gem_handle);
         link = link_copy.next;
      }
   }

   VG(VALGRIND_DESTROY_MEMPOOL(pool));
}

VkResult
anv_bo_pool_alloc(struct anv_bo_pool *pool, struct anv_bo *bo, uint32_t size)
{
   VkResult result;

   const unsigned size_log2 = size < 4096 ? 12 : ilog2_round_up(size);
   const unsigned pow2_size = 1 << size_log2;
   const unsigned bucket = size_log2 - 12;
   assert(bucket < ARRAY_SIZE(pool->free_list));

   void *next_free_void;
   if (anv_ptr_free_list_pop(&pool->free_list[bucket], &next_free_void)) {
      struct bo_pool_bo_link *next_free = if (!entry)
      return NULL;

   struct anv_cached_bo *bo = (struct anv_cached_bo *)entry->data;
   assert(bo->bo.gem_handle == gem_handle);

   return bo;
}

UNUSED static struct anv_bo *
anv_bo_cache_lookup(struct anv_bo_cache *cache, uint32_t gem_handle)
{
   pthread_mutex_lock(&cache->mutex);

   struct anv_cached_bo *bo = anv_bo_cache_lookup_locked(cache, gem_handle);

   pthread_mutex_unlock(&cache->mutex);

   return bo ? &bo->bo : NULL;
}

#define ANV_BO_CACHE_SUPPORTED_FLAGS \
   (EXEC_OBJECT_WRITE | \
    EXEC_OBJECT_ASYNC | \
    EXEC_OBJECT_SUPPORTS_48B_ADDRESS | \
    EXEC_OBJECT_PINNED)

VkResult
anv_bo_cache_alloc(struct anv_device *device,
                   struct anv_bo_cache *cache,
                   uint64_t size, uint64_t bo_flags,


true;

      val = old;
   }
}

void
anv_bo_cache_release(struct anv_device *device,
                     struct anv_bo_cache *cache,
                     struct anv_bo *bo_in)
{
   assert(anv_bo_cache_lookup(cache, bo_in->gem_handle) == bo_in);
   struct anv_cached_bo *bo = (struct anv_cached_bo *)bo_in;

   /* Try to decrement the counter but don't go below one.  If this succeeds
    * then the refcount has been decremented and we are not the last
    * reference.
    */
   if (atomic_dec_not_one(&bo->refcount))
      return;

                        WENDT v. LEONARD
GENERAL OF NORTH CAROLINA, Raleigh, North Carolina;
Claud Roberson Wheatly, III, WHEATLY, WHEATLY, NOBLES,
WEEKS & WAINWRIGHT, Beaufort, North Carolina; Janet Marie
Lyles, DAVIS, MURRELLE & LUMSDEN, Beaufort, North Caro-
lina; Robert Clifton Dodge, ROBERT C. DODGE, P.A., Beaufort,
North Carolina, for Appellees.

Unpublished opinions are not binding precedent in this circuit. See
Local Rule 36(c).

                              OPINION

PER CURIAM:

   Peter Wendt appeals the district court’s order dismissing his com-
plaint filed under 48 U.S.C. § 1983 (2000) and the denial of


to determine the average time to diagnosis and annual costs associated with various diagnostic algorithms for GD in a population of 100,000 managed care enrollees. Diagnostic algorithms used in current practice and hypothetical algorithms that include the TSI test were identified using published clinical guidelines and interviews with practicing endocrinologists. The model estimates costs of current and TSI test-based diagnostic algorithms using payment amounts for laboratory tests, procedures, and physician visits. Compared with non-TSI algorithms, 100% use of algorithms that include the TSI test result in 46% faster time to diagnosis and generate 47% overall cost savings due in large part to reductions in costly procedures and specialist office visits. Incorporation and early utilization of the TSI in vitro diagnostic test into current diagnostic algorithms confers cost savingsof Cigars which is now available in the App Store for iPhone®, and iPod Touch® and on Google Play™ for Android™. For more information head to http://drewdiplomat.com

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The number of distinct Legendrian rational unknots with tight complements is determined via the classification of tight contact structures on solid tori; this strategy has previously been employed by Etnyre [@etny]. We then describe the expected number of Legendrian rational unknots explicitly in a contact surgery diagram of the lens space. For the $3$-sphere, such a description is due to Plamenevskaya [@plam12]. In all cases the knots are distinguished by the rational analogues of the classical Legendrian knot invariants.

Here is an outline of the paper. In Section \[section:unknots\] we recall the topological classification of rational unknots in lens spaces. In Section \[section:classical\] we describe a result of Lisca et al. [@loss09] about the computation of the classical Legendrian knot invariants of a Legendrian knot presented in a contact surgery diagram. We extend theirBülent Tosun has been working on the classification problem discussed in this paper using a parallel approach, but staying closer to the argument in [@etny] rather than relying on surgery diagrams for the existence part of the classification. This may in fact be advantageous for dealing with the general $L(p,q)$.

Rational unknots in lens spaces {#section:unknots}
===============================

The lens space $L(p,q)$ with $p\in{\mathbb{N}}$ and $1\leq q\leq p-1$ coprime to $p$ is defined as the quotient space of $S^3\subset{\mathbb{C}}^2$ under the ${\mathbb{Z}}_p$-action generated by $$(z_1,z_2)\longmapsto ({\mathrm{e}}^{2\pi{\mathrm{i}}/p}z_1,{\mathrm{e}}^{2\pi{\mathrm{i}}q/p}z_2).$$ This gives $L(p,q)$ a canonical orientation, and our contact structures are assumed to be positive for that orientation. Alternatively, $L(p,q)$ with the described orientation can be obtained by surgery along a single $(-p/q)$-framed unknot in $S^3$.

A *rational unknot* $K$ in some $3$-manifold $M$ is a knot with a


not contained in the statement of their lemma, but in the paragraphs preceding it, and it is used implicitly in their argument.)

\[lem:loss\] The rational invariants of $L_0\subset(Y,\xi)$ are given by $${{\tt rot}}_{{\mathbb{Q}}}(L_0)={{\tt rot}}_0-\left\langle
\left(\begin{array}{c}{{\tt rot}}_1\\ \vdots\\ {{\tt rot}}_n\end{array}\right),
M^{-1}
\left(\begin{array}{c}{{\tt lk}}(L_0,L_1)\\ \vdots\\ {{\tt lk}}(L_0,L_n)\end{array}\right)
\right\rangle$$ and $${{\tt tb}}_{{\mathbb{Q}}}(L_0)={{\tt tb}}_0+
\frac{\det M_0}{\det M}.$$

These formulae are exactly the same as those in [@loss09], with ${{\tt tb}}$ and ${{\tt rot}}$ replaced by their rational counterparts. However, since it is not entirely clear where the order of $L$ in $H_1(Y)$ might or might not be relevant for the argument, we deem it worth to include a proof.

The relative Euler class
------------------------

Before we turn to that proof, we want to discuss the behaviour of the relative Euler class of a contact structure under a contact $(\pm 1)$-surgery along a Legendrianknot $L_i$. A neighbourhood of $L_i$ can be identified with a neighbourhood of $S^1\times\{0\}\subset S^1\times{\mathbb{R}}^2$, equipped with the contact structure $\ker(\cos\theta\, dx-\sin\theta\, dy)$. We think of $S^1\times D^2\subset S^1\times{\mathbb{R}}^2$ as the solid torus we cut out during the surgery. The boundary $S^1\times \partial D^2$ of this solid torus is a convex surface with two dividing curves $(\pm\sin\theta,\pm\cos\theta,\theta)$. These curves lie in the class of the longitude ${\lambda_{\mathrm{c}}}$ giving the contact framing. Write $\mu$ for the meridian of $S^1\times\partial D^2$ and $\lambda$ for the standard longitude $S^1\times\{*\}$. Then ${\lambda_{\mathrm{c}}}=\lambda-\mu$. Thus, in terms of the standard meridian and longitude $\mu,\lambda$, the slope of the dividing curves is $-1$. The convex torus $S^1\times \partial D^2$ has a linear Legendrian ruling given by the $\theta$-curves, which represent the class $\lambda=\mu+{\lambda_{\mathrm{c}}}$.

Write $\mu',\lambda'$ for meridian and


the contact structure determined up to isotopy by $d_3(\xi)=1/2$, and $$\bigl({{\tt tb}}(L),{{\tt rot}}(L)\bigr)\in\bigl\{(n,\pm(n-1))\co n\in{\mathbb{N}}\bigr\}.$$ These invariants determine $L$ up to coarse equivalence, and any pair of invariants in this set is realised.

Examples of Legendrian unknots in $(S^3,{\xi_{\mathrm{st}}})$ that realise the invariants stated in the theorem are given by arbitrary stabilisations of a standard Legendrian unknot with ${{\tt tb}}=-1$ and ${{\tt rot}}=0$.

Examples of exceptional unknots with the stated invariants have been described by Plamenevskaya [@plam12] in terms of the front projection of the knot in a contact surgery diagram, see Figure \[figure:olga-lens\].

$({\mathrm{a}})$ at 0 167 $({\mathrm{b}})$ at 0 55 $({\mathrm{c}})$ at 88 167 $L$ \[bl\] at 66 132 $+1$ \[l\] at 66 148 $+1$ \[l\] at 66 107 $L$ \[bl\] at 64 39 $+1$ \[l\] at 64 14 $L$ \[bl\] at146 39 $+1$ \[l\] at 146 14 $-1$ \[l\] at 146 58 $-1$ \[l\] at 146 76 $-1$ \[l\] at 146 132 $-1$ \[l\] at 146 150 ![The exceptional unknots in the $3$-sphere.[]{data-label="figure:olga-lens"}](olga-lens "fig:")

Each of these diagrams gives a copy of $S^3$, as can be seen by simple Kirby moves, cf. [@plam12]. A straightforward computation with the formula from Proposition \[prop:d3\] shows that each diagram gives a contact structure on $S^3$ with $d_3=1/2$. So this contact structure is overtwisted (and determined up to isotopy by this value of $d_3$ thanks to Eliashberg’s classification of overtwisted contact structures [@elia89], cf. [@geig08]). Contact $(-1)$-surgery along $L$ cancels the $(+1)$-surgery along the parallel knot, see [@dige04 Section 3] or [@geig08 Prop. 6.4.5]. This leaves us with a diagram containing only contact $(-1)$-surgeries, or one with a single $(+1)$-surgery along


tight $({\mathbb{R}\mathrm{P}}_3,{\xi_{\mathrm{st}}})$ with ${{\tt tb}}_{{\mathbb{Q}}}(L_0)=n+1/2$.

For $n=0$ the slope $s_2$ is infinite. This can be changed to $-1$ by a single Dehn twist. So there is a unique tight contact structure on $V_2$. For $n\geq 1$, it is easy to see inductively that the slope $s_2=-2-1/n$ has the continued fraction expansion $[-3,-2,\ldots ,-2]$, where $-2$ occurs $n-1$ times. So, by Giroux and Honda, there are three tight structures for $n=1$, and four each for $n\geq 2$. In all cases, this equals the number of examples in Figures \[figure:rp3-tb3\] and \[figure:rp3-tb5\].

The lens spaces $L(p,1)$ {#section:Lp1}
========================

The discussion of the preceding section easily generalises to the lens spaces $L(p,1)$. The following theorem subsumes Theorems \[thm:elfr\] and \[thm:rp3\]. Part (a) is essentially the same as [@baet12 Theorem 5.5]; again, we state it here merely for completeness and comparison      $\pm(n+\frac{2}{p}-\frac{2k}{p})$   $-\frac{(p-2k+2)^2}{4p}+\frac{3}{4}$

  : Invariants of the exceptional rational unknots in $L(p,1)$. \[table:Lp1\]

In order to illustrate the range of methods available, we prove overtwistedness of the contact structures on $L(p,1)$ represented in Figure \[figure:Lp1\] by a different argument for each of the three diagrams.

For Figure \[figure:Lp1\](a) we appeal to the classification of tight contact structures on lens spaces [@giro00; @hond00]. All these structures are Stein fillable. Now take $p-2$ additional parallel unknots and perform contact $(-1)$-surgery along them. This produces the diagram from Figure \[figure:rp3-tb3\](a), and hence an overtwisted contact structure on ${\mathbb{R}\mathrm{P}}^3$. If the original surgery diagram had produced a tight (and hence, in this particular case, Stein fillable) structure, the resulting structure on ${\mathbb{R}\mathrm{P}}^3$ would still be Stein fillable, and hence tight.

For


of ${\mathbb{R}\mathrm{P}}^3$ (in case (a) perform a $(-1/(p+1))$-surgery along $L$).

The argument that our list of examples is complete is very similar to the case of ${\mathbb{R}\mathrm{P}}^3$, and we only list a few of the necessary modifications. The gluing of $V_1$ and $V_2$ is now given by $\mu_2=-\mu_1+p\lambda_1$ and $\lambda_2=\lambda_1$. With ${\lambda_{\mathrm{c}}}=n\mu_1+\lambda_1$, $n\in{\mathbb{Z}}$, we get ${{\tt tb}}_{{\mathbb{Q}}}(L)=n+1/p$. The corresponding slope of $\partial V_2$ is $s_2=-p-1/n$.

For $n\leq -1$, there are $(p-1)\cdot|n|$ distinct contact structures on $V_2$. These correspond to the rational unknots in a tight $L(p,1)$.

For $n=0$ there is again a unique tight contact structure on $V_2$. For $n\geq 1$, the slope $-p-1/n$ has the continued fraction expansion $[-p-1,-2,\ldots ,-2]$, where $-2$ occurs $n-1$ times. So we have $p+1$ tight structures for $n=1$, and $2p$ each for $n\geq 2$.

The lens space $L(5,2)$ {#section:L52}
=======================

We        $6$

  : Number of Legendrian realisations of $K_1$ in $L(5,2)$. \[table:L52-numbers1\]

The cases with $n\leq -1$ correspond to a tight contact structure on $L(5,2)$ as follows. Realise $L(5,2)$ by contact $(-1)$-surgeries along a ‘shark’ and a standard ${{\tt tb}}=-1$ Legendrian unknot forming a Hopf link. A standard Legendrian unknot linked once with the shark gives a Legendrian realisation of $K_1$ with ${{\tt tb}}_{{\mathbb{Q}}}=-1+2/5$. Depending on a choice of orientation, this has ${{\tt rot}}_{{\mathbb{Q}}}=\pm 2/5$. By successive stabilisations of this knot, one obtains the $|2n|$ realisations with ${{\tt tb}}_{{\mathbb{Q}}}=n+2/5$.

The surgery pictures of the exceptional realisations of $K_1$ are given in Figures \[figure:L52K1a\] and \[figure:L52K1b\]; the invariants are listed in Table \[table:L52K1\]. The computations follow the same pattern as in the case of $L(p,1)$, so


anchoring their boats in anticipation of the typhoon

Media playback is unsupported on your device Media caption BBC Weather's John Hammond says Samar province is in the line of fire for the typhoon

Tacloban's Deputy Mayor Jerry Yaokasin told the BBC's Newsday: "We haven't yet fully recovered from last year's super-typhoon Haiyan and here we go again.

"It's like we're seeing a movie, it's like the Groundhog Day.

"And it's stirring up a lot of emotions in our hearts and bringing back so many painful memories of what happened during super typhoon Haiyan."

The Philippine weather authorities said that as of 16:00 local time on Friday (08:00 GMT) Hagupit was 370km (230 miles) east of Eastern Samar and moving at 13km/h, a relatively slow speed.

It has weakened slightly, but still remains powerful, withQ:

I see my clients in AD but not in WSUS

I set up a WSUS but dont see any clients in the Unassigned Computers group. I can find my clients in the ADAC, when I select myWSUS (local) > computers.
My group policy management got a domain myWSUS.local but I dont see the groups here, is this maybe the problem?
those are some of the errors i got in the windowsupdate log:
2015-07-29  03:02:27:702     852    86c Agent   ***********  Agent: Initializing global settings cache  ***********
2015-07-29  03:02:27:702     852    86c Agent     * Endpoint Provider: 00000000-0000-0000-0000-000000000000
2015-07-29  03:02:27:702     852    86c Agent


property as the value selected in the ddl.
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A:

One way to make it extensible is to make it reusable rather than stick it to one dropdown. You can even make it into a jQuery plugin so that it looks like this:
$('.someAutocompleteBox').dependentAutoComplete({

  /* the selector of the element to monitor changes */
  elementToMonitor : '.theElementToMonitor',

  /* value set, which correspond to the value of the previous input */
  sets : {
    drugs : DRUG_URL,
    hospitals : HOSPITAL_URL,
  }

  /* you can monitor depending on the event and which value to grab */
  triggeringEvent :


property earlier)
Update the current element's autocomplete source.

The plugin code (in the init) should look something like this:
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    short. Take a ride aboard Calypso, and you will be happy with the exciting ride that follows, filled with laugh-inducing fun on this good flat ride overall.

Located in a place that Ive never seen with anyone in it, Calypso is a decent ride, but nothing mindblowing. A good family flat ride, but if youve ridden one, youve ridden them all - and this one is no different.

This has got to be the most boring flat ride Ive ever been on. It was a merely a "tilted" scrambler. I really hope Cedar Point gets some high-tech, new flats over the next couple of years. I wouldnt mind seeing Calypso go. The only good thing is that the ride ops gave us 2 cycles. Too bad the ride wasnt worth


up with anyone who is doing more to shatter the myths about single mothers in the United States than Tim Casey, senior staff attorney at Legal Momentum, the nation’s oldest organization advocating on behalf of the legal rights of women and girls. Ad Policy

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Join the Single Parent Policy Advocacy Network (SPPAN) to educate and advocate for public policies to improve the economic security of single parents and their children. Simply send an e-mail with “subscribe” in the subject line to tcasey@legalmomentum.org.

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Playing Chicken with Workers’ Safety—Tell USDA to Withdraw Proposed Poultryof sustainable fish trade for coastal communities, particularly in developing countries.

To this end, this year’s Second Oceans Forum on the Trade-Related Aspects of SDG 14 will gather experts to analyze and share national experiences, and identify best practices around fisheries, trade and the environment. The objective of the Ocean Forum is to propose specific actions and policy recommendations for harnessing trade to conserve and sustainably use the oceans, seas and marine resources.

Learn more about UN Environment’s work on the green economy, and on trade.


In celebration of the 50th anniversary of Star Trek: The Original Series, Mattel will be showcasing an exclusive “Vina” Barbie Doll at the San Diego Comic-Con. The sexy character, made famous by actress Susan Oliver, appeared in the Star Trek pilot episode, “The Cage,” in 1965. Apparently the episode was not broadcast on television until 1988.

The episode is a cult classic and has a different captain, namely Christopher Pike. The story starts with the Enterprise crew receiving a radio distress call from the fourth planet in the Talos star group, where Captain Pike meets a beautiful young woman named Vina. She is a ruse of enemy forces, the Talosians, who seek to lure the Enterprise to their planet. Vina is presented to Pike in various guises and settings,Día de los Muertos: Learning About Death Through Observing and Pitching In.
The chapter explores how young children in the state of Puebla, Mexico are socialized with respect to death by observing and pitching in during the annual celebration for día de los muertos. This chapter focuses on observations made of children's participation in practices related to día de los muertos and their experiences with death as explored through ethnographic interviews of preschool children and adults from the cities of Cholula and Puebla. We found that children were included in all aspects of día de los muertos and participated by hanging out, observing, pitching in, and listening. Parents (and grandparents) viewed this active participation as crucial for children to acquire the skills and traditions necessary to be responsible adults


be time consuming and frustrating.
Prior art references available to applicant have not addressed the problem of installating wire harness clamps and the like. However, U.S. Pat. No. 1,440,377, Nut Holding Member, by L. F. Crumley attacked the problem of positioning a nut so it could be secured on a shaft in a confined area. Crumley discloses a forceps-like device having arms terminating in nut retainer halves. When the two halves are drawn together a nut can be positioned therebetween. The retainer halves are slotted so that a wrench can be inserted to tighten the nut on the shaft.
In U.S. Pat. No. 2,805,594, Nut-Holding Socket Wrench by A. Fogel, a conventional socket wrench is modified by the incorporation of a retractable retaining tab which protrudes into a slot inone wall of the socket. A nut can be installed in the socket by first withdrawing the tab from the slot and thereafter inserting the nut. Once released the tab frictionally holds the nut within the socket. This wrench has the advantage of allowing the nut to be installed using only one hand, but no means are provided to align the ends of a clamp and to force them toward each other prior to engagement with the nut.
Another patent of interest is U.S. Pat. No. 2,600,214, Adjustable Bolt-Holding Wrench by F. G. Davis. Davis discloses a C-clamp having sockets at each end of the C-member with one of these members being moveable. This sort of device allows both the nut and screw to be properly aligned with each


an appreciation for the best of cold things," says Clare Hamilton-Eddy, spokeswoman for 7-Eleven, where the slushy drinks are sold. "In Manitoba, more than anywhere else, it's a part of life."

The designation is bestowed based on the average number of Slurpee cups sold per store in a region, where Manitoba came out on top out of 16 countries. The sheer amount of Slurpees Manitobans have consumed to be awarded such a prestigious title is not available.

The 7-Eleven at the corner of Ness Avenue and Sturgeon Road sold the most Slurpees in the city, and has been the leader for about the last five years, manager Ali Mirza says.

"There's no flavour we've brought in that people don't like," he laughs, adding Dr. Pepper, Pepsi and grape are the mostJuly 11 (or 7/11), the convenience-store chain will hand out free Slurpees between 11 a.m. and 7 p.m., across the country in honour of the company's birthday, but only while the 7.11-ounce cups last.

jennifer.ford@freepress.mb.ca


exit the bus. No clue what hotel the visitors stay in though.

Yeah, pretty much like that everywhere. And I have been to 3 Steeler v Chiefs games down there - so been there for wins and losses. You always hear stories of how bad "_______" fans are at their stadium if you're the visitor, but it's almost always some idiot who wants to run his mouth or go beyond cheering into the taunting territory.

In Denver a few years back, I had to yell about a 12 rows down to tell another Steeler fan to cool off because I didn't want to get my ___ kicked. Some Broncos fan was like, "You're cool man, we'll only kick his as long as you look the other way!" That actually diffusedhigh-potency of vitamin E is Plunkett's Vita E Natural Vitamin E Cream, which is also infused with rosehip oil to promote skin rejuvenation.

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would love to figure out how to limit it to specific wp imports
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then § 1958(b) defines a phrase with no application to the substantive offense, and leaves undefined the phrase that does appear in the substantive law.5 We note that the question we settle today will have little importance going forward, as Congress has recently amended the statute to eliminate any confusion over the scope of § 1958(a).

III.

11
As a result, even though Perez's calls to Casiano were wholly intrastate communications, the fact that they were made using the SNET network, a facility involved in interstate commerce, leads us to conclude that Perez was properly subject to prosecution for using interstate commerce facilities in the commission of murder-for-hire. Accordingly, we AFFIRM the judgment of the district court.

Notes:

1
 The five counts were:

1
 Conspiracy to commit murder-for-hire involving interstate travel or the use


on a train wreck that is the American Dream for 9-10 songs, depending on what version you've got.

Eight years after their debut and hiatus, they did a one-off reunion show in 2010. Two years after that though, that one-off show would prove to be the start of their actual reunion. In 2012 they began touring again, and recorded and released a slew of singles, which they put out on their website. These songs were the first new ones written and recorded since Read Music/Speak Spanish. Though the last of them was released in 2013, they were also included on 2015's Payola, which is just what we've finally been graced with. This is their long-awaited sophomore album, which features 6 previously released tracks, and 8 new ones. Needless tothe printing or apply a surface varnish processing during or after printing and the cost becomes very high as compared with a normal printed matter.
An object of the present invention is to provide a thermoplastic resin film ensuring ink adhesion in a printed matter obtained by gravure printing, flexographic printing, letter press printing, offset printing or the like and moreover, imparting scratch resistance to the printed matter.


terms of the contract of carriage. Conagra filed the present suit to recover damages associated with the wheat spill. The case is currently before this Court upon motions for summary judgment filed by both parties.
Paragraph 2(b) of the bill of lading issued by Burlington Northern to Conagra contains the following language:
As a condition precedent to recovery, claims must be filed in writing with the . . . carrier on whose line the loss, damage, injury or delay occurred, within nine months after delivery of the property; . . . and suits shall be instituted against any carrier only within two years and one day from the day when notice in writing is given by the carrier to the claimant that the carrier has disallowed the claim . .an aircraft cable (clips provided), snaked up the center, or pulled tight into a straight line up the center to create various looks.

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How often do


not solvable [@Aharony:2003sx]. On the other hand, large $N$ vector models whilst solvable, lead to at best weakly interacting dynamics and possessing nearly conserved higher spin currents. In recent years a new possibility has arisen: melonic models which appear to provide a happy middle ground of being technically tractable and having non-trivial dynamics.

Motivated by these considerations, we will attempt to construct large $c$ interacting two-dimensional CFTs. One approach would be to study a family of theories with central charge $c$ as a parameter which can be dialed appropriately. For instance, the D1-D5 CFT is obtained as (deformation of) a symmetric product CFT [@Strominger:1996sh], the sigma model with target $X^N/S_N$ where $X$ is either $K3$ or $T^4$ in the large $N$ limit ($c\sim N$). Another possibility is to takescaling limits of a family of WZW coset models [@Gaberdiel:2010pz] (or even WZW models themselves [@Kiritsis:2010xc]). The aforementioned examples however end up being the analog of vector-like modes; in the large $N$ limit such theories typically have higher spin symmetry. For the orbifold example with sufficient supersymmetry one has a moduli space: far out away from the orbifold point, one expects to recover semiclassical gravity. Given this status quo, we seek to ask if we can conjure up interesting CFTs, exploiting lessons learnt from the analysis of theories with melonic structure.

While field theories with melonic large $N$ expansions have been studied in the literature for a while, recent interest in them owes to similar structures being relevant for the analysis of the disordered Sachdev-Ye-Kitaev (SYK) model [@Sachdev:1992fk; @Kitaev:2015aa;


valued set of matrices which can be used to construct matrix-vector models, cf., [@Ferrari:2017ryl] who motivated such models by imagining the D0-brane matrix model with a large number of transverse dimensions. In this case, one can explicitly view the melonic diagrams as a subset of standard planar diagrams (by considering ribbon graphs decorated with an internal line corresponding to the vector label).

Now $\mathcal{N}=(2,2)$ models in two dimensions are well studied in the literature as they play a central role in mirror symmetry through the LG/Calabi-Yau correspondence [@Martinec:1989in; @Vafa:1988uu; @Greene:1988ut] cf., [@Witten:1993yc; @Hori:2003ic] for detailed reviews. The general idea of $(2,2)$ LG models is that we have a non-trivial RG flow driven by a relevant superpotential. The IR dynamics is altogether controlled by the superpotential, so one expects tostates [@Bulycheva:2017ilt; @Choudhury:2017tax]). Two natural possibilities come to mind: either gauge the symmetries to focus on the singlet sector, or consider explicit breaking of the symmetry whilst retaining solvability.

We will demonstrate that the most efficacious choice is to break the symmetry by considering *anisotropic tensor models*. These will have tensor valued fields with index contractions inspired by the tetrahedral structure, except that we will bias individual contractions with slightly different couplings. By a judicious choice of the couplings we will show that the theory retains large $N$ solvability, which we illustrate explicitly for weak anisotropy, where we can use perturbative arguments. It will be important to note that the anisotropic couplings are specified once and for all in the microscopic Lagrangian, and so we are dealing with a


its cousin the matrix-vector model. It is worth noting that the matrix-vector model has some nice features in that we can identify the melonic diagrams as a subclass of planar diagrams with an internal vector ‘decoration’. One can view this as arising from a kind of Veneziano limit [@Veneziano:1976wm] where we scale the ‘flavor’ degrees of freedom commensurately with the ‘color’ degrees of freedom in the planar large $N$ expansion.[^5] It has the advantage of making certain aspects of the large $N,M$ counting more transparent. We should note that a similar philosophy has been advocated earlier in [@Ferrari:2017ryl]. These constructions were inspired by the D0-brane matrix model where the adjoint valued scalars carry a spacetime index; [@Ferrari:2017ryl] wished to view these theories as matrix models on branes livingfour-point function at inverse temperature $\beta$ that probes the scrambling and chaotic dynamics of the theory. Thermal correlation functions can be conformally mapped to vacuum correlation functions on $\bR^2$. Using this map, it follows that the chaos limit for the out-of-time-ordered Lorentzian thermal four-point function is equivalent to the Regge limit of an analytically continued vacuum four-point function [@Murugan:2017eto]. By this relation, the chaos exponent can be easily computed using the eigenvalue of the kernel . Analytically continuing the spin in the $n^{\rm th}$ Regge trajectory to intersect the principal series at h=[12]{}(1+),|[h]{}=[12]{}(1-), we obtain the Regge intercept $\ell_n$. The chaos exponent $\lambda_L$ is related to the leading Regge intercept by \_L = (\_0-1)[2]{}. For our model, the leading Regge intercept is roughly \_01.55, which leads to a


We then rewrite the integrand as I\_[h,|[h]{}]{}(,) = (-1)\^[|[h]{}-h]{} (h) (|[h]{}) , \[eq:integrand\_rewrite\] to make the singularity structure manifest. For one, the function ${\varphi_{h}(\chi)\over \Gamma(h)}$ has no poles and its zeros are not at $h\in {1\over 2}\bZ$. Therefore, the poles and zeros of the integrand $I_{h,\bar{h}}(\chi,\overline\chi)$ come from $\frac{\sin \pi h}{\cos \pi \bar{h}}\Gamma(h)\Gamma(\bar{h})$, which are summarized as &[poles]{}:|[h]{}+, \_[0]{},\
&[zeros]{}: h\_[1]{}. \[eq:poles+zeros\] Since we close the contour so that $u = is \in \mathbb{R}_{\geq 0}$, we are interested in the following domain in the $(h,\bar{h})$ plane: h-|[h]{},h+|[h]{}0. \[eq:confdimrestriction\] Therefore, we are only interested in the poles at (h,|h)=(0,0)(h,|h)([12]{},[12]{})+\^2, (h+|[h]{}0). \[eq:polesofinterest\] As discussed previously, we deform the contour to avoid the pole at $(h,\bar h)=(0,0)$.

It remains to show that the residues of the poles at $(h,\bar h)\in ({1\over 2},{1\over 2})+\bZ^2$\_[b\_[1]{},b\_[2]{},b\_[3]{}]{}\_[c\_1b\_[1]{},c\_2 b\_[2]{},c\_3 b\_[3]{}]{} \^[c\_1b\_[2]{}b\_[3]{}]{} \^[b\_[1]{}c\_2b\_[3]{}]{} \^[b\_[1]{}b\_[2]{}c\_3]{}, where we have used the symmetry to simplify this expression. Then we state the claim that $\mathcal{M} = \{\mathbf{0}\}$ as follows:\
****: There exist nonzero $\A_{a_{1}b_{1},a_{2}b_{2},a_{3}b_{3}}$ such that the set of equations \[eqn:nomoduli\_claim\] {\_[c\_1c\_2c\_3]{} = 0|1 c\_1,c\_2,c\_3 N} has no non-trivial solution.\
We shall provide a sketch of the proof below relegating technical details to Appendix \[sec:nomoduliproof\]. The idea is to convert this set of non-linear equations to a linear algebra problem. This can be done by working in the space of monomials built from the components of our tensor field. We have $N^3$ equations given by the zero sets of the polynomials $\mathfrak{f}_{c_1c_2c_3}$, each of which is a linear combination of degree $3$ monomials in the $N^3$ variables $\mathscr{X}^{a_1a_2a_3}$. We however have many more


the deformed superpotential in some detail. We proceed by first exhibiting that the theory with gauge group ${\rm SU}(N)$ has a non-compact Coulomb branch, which however can be lifted if we consider the group ${\rm PSU}(N) \cong {\rm SU}(N)/\mathbb{Z}_N$. We will find that for specific odd/even parity choices of $N,M$ and suitable choices of bare theta angles, we can end up with a compact Coulomb branch. The real issue for us is whether we have a compact Higgs branch. This turns out to be the case for some specific choices such as $M=1$, $N$ arbitrary, or $M=N=2$. For $M=N=3$, we numerically found nontrivial solutions to the equations for generic $\A_{IJ}$. More precisely, we numerically minimized a modified potential V(Y,Y) = & |g|\^2\_[I,J,K=1]{}\^M\_[IJ]{} \_[KJ]{}\^\* ( Y\^I Y\^J Y\^I Y\^Kanalysis, we find it easier to work in the simplified case where each $Y^{I}$ is traceless: ${\rm Tr}(Y^I) = 0$ for every $1 \leq I \leq M$. Some basic results for $\mathcal{P}_\mathcal{R}(y)$ for the traceless model are tabulated below in Table \[tab:Hpoin\]. We have always chosen the $R$-charge to be that given by the IR fixed point value for a quartic superpotential $R = \frac{1}{2}$ to facilitate comparison, We see that the unconstrained count for the free theory, which of course has an infinite-dimensional chiral ring, gets somewhat reduced by the $F$-term constraints, but generically this reduction does not seem strong enough to cull down the ring to a finite one even with the most generic superpotential. Curiously, however, the generic superpotential ends up culling a lot of states


                generic $W$              $1+6\, y^\frac{1}{2}+8\, y^\frac{3}{4}+21\, y+51 \, y^\frac{5}{4}+64\, y^\frac{3}{2}+71\, y^\frac{7}{4}
                                                                                This provides checks and a bit more insight on some of our conclusions on the general structure of the Coulomb and Higgs branches.

The computation of the elliptic genus for $\mathcal{N}=(2,2)$ theories was first described in [@Witten:1993jg] for Landau-Ginzburg models. Recently, [@Benini:2013nda; @Benini:2013xpa] used localization techniques to give general expressions for the elliptic genus of ${\cal N}=(2,2)$ gauged linear sigma models. We will mostly use their results and check the elliptic genus for rank-$1$ theories.

The elliptic genus is a Hilbert space trace over the Ramond-Ramond sector of the IR SCFT, explicitly defined by $$\mathcal{Z}(q, y, \{x_a\} ) = {\rm Tr}_{\text{RR}} \left( (-1)^F \, q^{\Delta_L} \, \bar{q}^{\Delta_R} \, y^{J_L}
\right),
\label{eq:egenus}$$ where $J_L$ is the ${\rm U}(1)_L$ charge for the left-moving $R$-symmetry. The parameters $q,\bar{q}$ encode the inverse temperature and the rotation


from $\theta_1(q,y^{\frac{1}{4}}x^{-2})$.

The non-compact Coulomb branch is again manifested by the singular behaviour of the $\chi_y$-genus. One can more simply examine the Witten indices to confirm this. They are given by $$W_\text{RR}\bigg|_{M=2} = -\frac{5}{2} \,,  \qquad W_\text{RR}\bigg|_{M=3} = \frac{61}{2} \,,  \cdots
\label{eq:}$$

#### Case III (${\rm PSU}(2)$ arbitrary $M$):

The situation with ${\rm SU}(2)$ gauge theory is that we have a non-compact Coulomb branch giving rise to some of the singular features seen above. Our discussion in §\[sec:cbranch\] and §\[sec:hbranch\] leads us to believe that the moduli space is compact when we consider gauging ${\rm PSU}(2) \cong {\rm SO}(3)$ in a theory with an anisotropic superpotential.

The computation for the elliptic genus can then be adapted from the results of [@Kim:2017zis]. It is given by $$\begin{split}
\mathcal{Z}(\tau, z) & =
z)\, \sin\pi(u+\frac{3}{4}\, z) }{\sin\left( \frac{\pi}{4}z\right)
    \, \sin\pi(u+\frac{1}{4}\, z)\sin\pi(u-\frac{1}{4}\, z)}\right)^M,\\
\chi_-(z)&=
    \frac{1}{4\, \cos\pi z}\left(- \frac{\cos \left(\frac{3\pi}{4}z\right)}{ z \,\cos \left(\frac{\pi}{4}z\right)}\right)^M .
\end{split}
\label{eq:chiyo3}$$ This is in perfect agreement with our analysis of Higgs and Coulomb branches. For specific values of $M$ and choices of the bare theta angle, $\theta_\text{bare}$, we have $$\begin{aligned}
&\chi_y=0&&{\rm for}~M=1,~\theta_{\text{bare}}=\pi,
\nonumber \\
&\chi_y=-1&&{\rm for}~ M=2,~\theta_{\text{bare}}=0,
\nonumber \\
&\chi_y=y^{-{3\over 4}}+6y^{-\frac{1}{4}}+1+6y^{\frac{1}{4}}+y^{{3\over 4}}&&{\rm for}~ M=3,~\theta_{\text{bare}}=\pi.
\label{eq:chiyspeco3}\end{aligned}$$ The Witten indices are also likewise commensurate; we obtain integral answers for the expected cases where the moduli space is compact. To wit, &\_ = 0&:&,-1,[312]{},-202,,\
&\_ = &:&0,-[32]{},15,-[4052]{},. \[eq:windo3\]

Discussion {#sec:discussion}
==========

The main thrust of our analysis was to construct large central charge CFTs in two spacetime dimensions, exploiting the large $N$ solvability of melonic theories. The advantage of the melonic dominance, as is by now well known,


and an anisotropic fixed point [@Fei:2015oha]. For $N>4$, the anisotropic fixed point is IR stable, and all the other fixed points can flow to it by turning on relevant deformations. However, this anisotropic fixed point lies outside the purview of large $N$ techniques, for at this fixed point the anisotropy parameters are not all of the same order in the large $N$ limit.

It is a pleasure to thank Kentaro Hori, Veronika Hubeny, Igor Klebanov, Emil Martinec, Shiraz Minwalla, Sun Woo Park, Cheng Peng, Douglas Stanford, Cumrun Vafa, Johannes Walcher, Edward Witten, and Xi Yin for illuminating discussions. We would like to thank KITP, UCSB for hospitality during the workshop “Chaos and Order: From strongly correlated systems to black holes”, where the research was supported in part by thehas codimension-$0$ in $\mathbb{C}^{N^{6}}$. Therefore, $V(D_{N^3-1})$ cannot contain $B_{\epsilon}^{+}(\mathbf{1})$. This immediately can be used to infer that $B_{\epsilon}^{+}(\mathbf{1}) - \left(B_{\epsilon}^{+}(\mathbf{1}) \cap V(\mathfrak{D}_{N^3-1}) \right) \neq \emptyset$, and hence we can make the desired choice of $\{\alpha_{a_{1}b_{1},a_{2}b_{2},a_{3}b_{3}}\}$.

Moduli for partial anisotropy
-----------------------------

Our discussion thus far has established that we are able to make a choice of the deformation parameters which lifts all the moduli. Let us look at some special cases to see what forms of anisotropy are needed for us to succeed in our quest. The key observation relies on noting that the proof has two crucial elements.

Firstly, the proof hinged on the fact that each partial derivative $\mathfrak{f}_{c_1 c_2 c_3} = \partial W_{4}/\partial \mathscr{X}^{c_1 c_2 c_3}$ contains the term $\left(\mathscr{X}^{c_1 c_2 c_3}\right)^{3}$ so that every diagonal element of the matrix


f^c_{a_p b}\, \mathcal{T}_{a_1 a_2\ldots a_{p-1} c a_{p+1} \ldots a_m} =0$ (we assumed for simplicity $\omega_a(t^b) = \delta_a^b$). One can alternately view them as being built from the $N$ independent Casimirs of $SU(N)$ along with the structure constants.

[^17]: We actually will not need the resultant, but a closely related, simpler polynomial which has the resultant as its divisor.
more than three months.

Ongoing use of medications known to influence glucose, i.e. sulfonylureas, growth hormone, metformin, anticonvulsants, thiazide or potassium depleting diuretics, beta adrenergic blockers, niacin. Subjects on such medications should be changed to a suitable alternative, if available, and will become eligible one month after medication is discontinued.

Choosing to participate in a study is an important personal decision. Talk with your doctor and family members or friends about deciding to join a study.
To learn more about this study, you or your doctor may contact the study research staff using the Contacts provided below.
For general information, see Learn About Clinical Studies.

Please refer to this study by its ClinicalTrials.gov identifier: NCT00419562


a good match today. Coming back from an early break in the 1st set and coming from behind in the second set (she was 4-0 down). Finished the match right on time before the rain really came down heavily.Q:

MVC 4 view model validation attribute - string length - error

I have this property on the MVC5 viewmodel with the StringLength validation attribute:
        [Required]
        [StringLength(4, MinimumLength = 4, ErrorMessage = "The postcodes must be 4 characters long.")]
        [Display(Name = "Postcode (four digits)")]
        public int Postcode { get; set; }

The client-side validation works, but when I execute the action by submitting the form I am getting this error:
Unable to cast object of type 'System.Int32' to type 'System.String'.

I know it is the attribute that's causing this because everything works when I comment out the [StringLength] attribute.
I suspect that this is


ALM Pip Slope.

The new rack is starting to take shape, but I have hit a bit of a snag! The case (made by Tip Top Audio) isn’t deep enough to house my Mark 1 Z3000 oscillator (also made by Tip Top Audio)! So it’s a good job I bought the Mark 2 version.

More selling on ebay methinks!

Also looking to get a Mutable Instruments Ears module soon to trigger my Rings module, as ably demonstrated in this video…

Decided to have a major upgrade of my studio and also try and fully integrate the modular with my laptop setup.

First purchase was the Maschine Jam which has really renewed my love for Maschine and should elevate it beyond the role of ‘just’ a drum machine.

I then ordered some Expert Sleepers ES-40,minister. And I'm hoping some way we're going to find a way through this."

'Great confidence' in Trudeau: Yukon MP

McLeod said it's important to hear more people testify before the justice committee before drawing any firm conclusions — something echoed by the North's other Liberal MP, Yukon's Larry Bagnell.

Bagnell said he's confident the justice committee and the ethics commissioner will get to the bottom of things.

Yukon MP Larry Bagnell says he's confident the justice committee and the ethics commissioner will get to the bottom of what may have gone on during Wilson-Raybould's time as justice minister and attorney general. (Mike Rudyk/CBC)

"We learned a lot [Wednesday], which I thought was great. And the ethics commissioner is independent of Parliament, so I think that's very good. And I look forward to


important components of the ECS, and measured depressive-like behaviors and synaptic protein expression following rTMS. Furthermore, we measured the expression levels of several components of the ECS system in hippocampal-derived astrocytes and neurons exposed to repetitive magnetic stimulation (rMS) with different parameters (5 or 1 Hz, 0.84 or 1.26 Tesla). Interestingly, we found that only high-frequency rTMS ameliorated depressive-like behaviors and normalized the expression of hippocampal synaptic proteins in CUS-treated rats; this effect was eliminated by knockdown of DAGLα or CB1R. Moreover, we found that rMS at 5 Hz increased the expression of DAGLα and CB1R in hippocampal astrocytes and neurons. Collectively, our results suggest that high-frequency rTMS exerts its anti-depressant effect by up-regulating DAGLα and CB1R.Parinda, 1942 A Love Story and Mission Kashmir.

Well, it’s his dream project and why shouldn’t it be? Have a look at the ensemble cast (he has never handled so many stars at the same time before). Amitabh Bachchan plays the title role, Sanjay Dutt, Saif Ali Khan, Boman Irani, Jackie Shroff, Sharmila Tagore, Vidya Balan, Jimmy Sheirgill, Raima Sen among others.

“Yes, it is an ensemble cast and I had reason enough to rope them in. I did not go for names, but went by characters that needed such actors,” justifies Chopra who directs Bachchan for the first time.

And yes, “The script was written keeping Bachchan in mind, yet, it is not just Bachchan centric. Every character has an important role to play,” adds Chopra who says, “Eklavya will


Duramycin (a negative tracer control; n = 3), or 99mTc-Annexin-V (a positive tracer-control; n = 4) were intravenously administered 30 min after reperfusion. Of the 10 Duramycin group animals, 4 animals were treated with an antiapoptotic agent, minocycline at the time of reperfusion. In vivo and ex vivo micro-single-photon emission computed tomography (μSPECT) and micro-computed tomography (μCT) imaging was performed 3 h after reperfusion, followed by quantitative assessment of tracer uptake and pathological characterization. Fluorescent Duramycin and Annexin-V were injected in 4 rats to visualize colocalization in infarct areas in a 40-min left coronary artery occlusion and 30-min reperfusion model. Intense uptake of Duramycin and Annexin-V was observed in the apical (infarcted) areas. The percent injected dose per gram uptake of Duramycin in apical region (0.751 ± 0.262%)leaks, the people around you probably know. So, even if it can’t be proven, it will be much harder for you to keep getting work in the field if you are known as the person who spills the beans.

It’s definitely not fool-proof. Anyone can really mention anything at any time, even accidentally in casual conversation, but all of that is verbal. As for physical media, it’s very rare for actual footage to get out. Many studios have policies forbidding phones or cameras in the open at the workplace. In addition, most studios can track USB use (we knew the story of one fellow who plugged in a cable to get some reference material off of Google and got promptly fired).

As I know this is a Star Wars themed


have access to entire season.

TLDR? Unless you have in a position of power in the set, you likely don’t have access to the script, and as I’ve said in almost each answer, if you do have access to the script, you’re not leaking it since it will be pretty easy for the powers that be to trace it back to you.

KL – Similar to the last question, the only people with access to entire scripts and footage are producers, director, editor, cinematographer, audio…. The actors will usually see all the footage, too. Point is, very very very few people will have access to both. Only the top, only the ones with the tightest-lips. The chances of this leaking are slim to none unless coming from post-production, but IWestern Empire in the 420s as magister militum of the Western Roman Empire. He served under the usurper Joannes until his death in a military uprising in Gaul in 425.

References

Category:5th-century Romans of Gothic descent
Category:Ancient Roman generals
Category:Scythian people
Category:Gothic warriors
Category:Magistri militum
Category:425 deaths
Category:Year of birth unknown
Category:Flavii


$200.00 to the appellant Johnson.  Both of the appellants denied sharing in the girls' earnings.

6
Each appellant raises three identical issues on appeal.  Appellant Johnson raises an additional issue which will be dealt with in the final section of the opinion.

ISSUES

7
I. Was the evidence sufficient to support a verdict of guilty as to each appellant?

8
II. Is the Mann Act unconstitutional as invidiously discriminatory on the basis of sex?III. Did outside influences deprive the appellants of a fair trial?

9
IV. The Johnson appeal.

I.

10
Appellants' primary contention is that the evidence was insufficient to conclude that the trip was "for the purpose of prostitution."  On this element, they both concede that the requisite intent may be proved by circumstantial evidence and that such evidence may include the conduct of theparties both before and within a reasonable time after the transportation.  See United States v. Snow, 507 F.2d 22 (CA7 1974); United States v. Tyler, 424 F.2d 510 (CA10 1970), cert. denied 400 U.S. 839, 91 S.Ct. 78, 27 L.Ed.2d 73.  See also United States v. Szymanski, 431 F.2d 946 (CA9 1970).

11
The appellants principally rely upon United States v. Tobin,426 F.2d 1279 (CA7 1970), which held in dictum that the mere fact that the female engages in prostitution at the end of the trip is not sufficient to satisfy the purpose element.  We do not quarrel with this as a general proposition, but find that there are several additional facts here.  Initially, one of the girls thought that she had informed the appellants of


her occupation.  Without purporting to be exhaustive, we also note that other events surrounding the departure from Portland, e. g., that appellants picked up the girls near a known prostitution area, that the girls paid no part of the trip expenses, and that the appellants told the girls that they could get bigger and better things in Yakima, are also significant.  Moreover, the events occurring in Yakima were not so remote as to preclude jury determination of the requisite intent from the outset, e. g., that the girls both engaged in prostitution on the night of arrival, that they were introduced on the same night to another prostitute who was to help the younger girl learn the ropes, and that both of the appellants shared inreturn a 'Input' class as defined in include\SFML\Window\Input.hpp
I believe you would typically call GetInput() on the SFML Window class.
So maybe all you wanted was game.h to instead have:
const sf::Input& GetInput() { return _mainWindow.GetInput(); }

I think you would do well to focus on C++ as a language before diving so deep into game programming.  If game programming is all you are interested in, you may want to look into higher level technologies that will let you make games.  Going down the C/C++ road without investing in understanding the language is likely to cause you enough pain that you will end up hating what you are doing, which would be unfortunate.


green ear yield in six commercial processing sweet corn hybrids \[[@pone.0223107.ref016]\]. Crowding stress tolerant sweet corn could be grown at higher plant densities than current densities. Consequently, the production gap---the difference in performance between using current and optimum plant densities---can be narrowed.

There is extensive literature on field corn plant density interactions with yield and yield components. In contrast, the inference space of the few studies on plant density and yield relationships in sweet corn is limited by a narrow range of environments in which field trials were conducted (e.g. up to 3 years at one location). An experimental approach that captures greater diversity in the conditions in which the crop is grown, including environments and management systems, would provide more valuable insight. Moreover, existing literature mostly investigates optimumcurrent plant density to gross profit margin-optimized plant density resulted in a subtle, yet statistically significant decline in ear number and ear mass by 0.08 ears plant^-1^ and 0.06 kg plant^-1^, respectively. Filled ear length showed a reduction (mean of 0.8 cm) compared to average ear length (mean of 0.5 cm) on shifting from current to gross profit margin-optimized plant density. Linear regression analysis showed ear number per plant decreased below 1.0 with increasing plant density ([S1 Fig](#pone.0223107.s001){ref-type="supplementary-material"}), indicating loss of marketable ears. Similarly, average ear length and filled ear length also decreased linearly with increasing plant density. More plants with unfilled ears at higher plant densities resulted in lower kernel mass, hence, lower case production and gross profit margin.

10.1371/journal.pone.0223107.t004

###### Effect of a crowding stress tolerant hybrid on


Minnesota and Wisconsin have ranged from 45,000 to 54,300 plants ha^-1^ \[[@pone.0223107.ref023], [@pone.0223107.ref024]\]. Two decades later, surveys of growers' fields showed slight change in plant density \[[@pone.0223107.ref016]\]. Our results demonstrate that, regardless of the processor variable, current plant densities are too low for CST sweet corn, by 10,100 to 18,200 plants ha^-1^. These results are consistent with previous studies in field corn that reported increased CST in modern hybrids allows using higher plant densities than their predecessors \[[@pone.0223107.ref003], [@pone.0223107.ref025], [@pone.0223107.ref026], [@pone.0223107.ref027]\].

Our results reveal that both processors and their contract growers will benefit from using gross profit margin-optimized plant densities of a CST hybrid like DMC 21--84. Overall green ear mass and case production increased by an average of 1.13 Mt ha^-1^ and 75 cases ha^-1^, respectively. Furthermore, these---
abstract: 'In this paper a countable family of new compactly supported [*non-Haar*]{} $p$-adic wavelet bases in ${{{\mathcal L}}}^2({{\mathbb Q}}_p^n)$ is constructed. We use the wavelet bases in the following applications: in the theory of $p$-adic pseudo-differential operators and equations. Namely, we study the connections between wavelet analysis and spectral analysis of $p$-adic pseudo-differential operators. A criterion for a multidimensional $p$-adic wavelet to be an eigenfunction for a pseudo-differential operator is derived. We prove that these wavelets are eigenfunctions of the fractional operator. In addition, $p$-adic wavelets are used to construct solutions of linear and semi-linear pseudo-differential equations. Since many $p$-adic models use pseudo-differential operators (fractional operator), these results can be intensively used in these models.'
address:
- 'International Center for Mathematical Modelling in Physics and Cognitive Sciences MSI, Växjö University,


papers [@Kh-Sh-Sk], [@Al-Ev-Sk], in [@S-Sk-1] all compactly supported wavelet Haar bases were constructed.

It turned out that the above-mentioned $p$-adic wavelets are eigenfunctions of $p$-adic pseudo-differential operators [@Al-Kh-Sh3]–[@Al-Kh-Sh5],  [@Kh-Sh1], [@Kh-Sh2], [@Koz0], [@Koz2] (see also Sec. \[s4\]). Thus the spectral theory of $p$-adic pseudo-differential operators is related to the wavelet theory. On the other hand, it is well-known that numerous models connected with $p$-adic differential equations use pseudo-differential operators (see [@Kh2], [@Koch3], [@Vl-V-Z] and the references therein). This is closely related to the fact that for the $p$-adic analysis associated with the mapping ${{\mathbb Q}}_p \to {{\mathbb C}}$, the operation of differentiation is [*not defined*]{}, and as a result, many models connected with $p$-adic differential equations use pseudo-differential operators, in particular, the fractional operator $D^{\alpha}$ (see the above-mentioned papers and books). These two facts imply that study of wavelets is importantwas introduced in the preprint [@Kh-Sh1] (for the brief review see [@Kh-Sh2]). In contrast to (\[62.0-1\]), for the basis (\[62.1\]) the number of generating wavelet functions is not minimal, for example, for $p=2$ we have $2^{m-1}$ wavelet functions (instead of one as it is for (\[62.0-1\]) and for classical wavelet bases in real analysis). The basis (\[62.1\]) is the [*non-Haar*]{} wavelet basis, since it cannot be constructed in the framework of the $p$-adic Haar MRA (see [@S-Sk-1] and Theorem \[th2\]). According to Remark \[rem1\], Kozyrev’s wavelet basis (\[62.0-1\]) is a particular case of the basis (\[62.1\]) for $m=1$. According to the same remark, our non-Haar wavelet basis (\[62.1\]) can be obtained by using the algorithm developed by the Benedettos [@Ben-Ben]. However, using our approach, we obtained the [*explicit formulas*]{} (\[62.1\]) for this basis. Moreover,


$\int_{B^n_{N}}\phi(x)\,d^nx=0$, iff  $\psi=F^{-1}[\phi]\in {{{\mathcal D}}}^{-N}_{-l}({{\mathbb Q}}_p^n)\cap\Psi({{\mathbb Q}}_p^n)$, i.e., $\psi(\xi)=0$, $\xi \in B^n_{-N}$.

Suppose that $\Phi'({{\mathbb Q}}_p^n)$ and $\Psi'({{\mathbb Q}}_p^n)$ denote the topological dual of the spaces $\Phi({{\mathbb Q}}_p^n)$ and $\Psi({{\mathbb Q}}_p^n)$, respectively. We call $\Phi'({{\mathbb Q}}_p^n)$ the space of $p$-adic [*Lizorkin distributions*]{}. The space $\Phi'({{\mathbb Q}}_p^n)$ can be obtained from ${{\mathcal D}}'({{\mathbb Q}}_p^n)$ by “sifting out” constants. Thus two distributions in ${{\mathcal D}}'({{\mathbb Q}}_p^n)$ differing by a constant are indistinguishable as elements of $\Phi'({{\mathbb Q}}_p^n)$.

We define the Fourier transform of $f\in \Phi'({{\mathbb Q}}_p^n)$ and $g\in \Psi'({{\mathbb Q}}_p^n)$ respectively by formulas $\langle F[f],\psi\rangle=\langle f,F[\psi]\rangle$, for all $\psi\in \Psi({{\mathbb Q}}_p^n)$, and $\langle F[g],\phi\rangle=\langle g,F[\phi]\rangle$, for all $\phi\in \Phi({{\mathbb Q}}_p^n)$. It is clear that $F[\Phi'({{\mathbb Q}}_p^n)]=\Psi'({{\mathbb Q}}_p^n)$ and $F[\Psi'({{\mathbb Q}}_p^n)]=\Phi'({{\mathbb Q}}_p^n)$ [@Al-Kh-Sh3].

Recall that in the real setting the Lizorkin spaces were introduced in$s\in J_{p;m}$. In order to construct the wavelets (\[62.1\]) by using the algorithm of [@Ben-Ben], we set $$\Omega_{s,0}=B_0\big(p^{-m}(s_{1}p+\cdots+s_{m-1}p^{m-1})\big)
\qquad\qquad\quad$$ $$\qquad
=p^{-m}(s_{1}p+\cdots+s_{m-1}p^{m-1})+B_0\subset B_{m-1},$$ i.e., remove the term $s_0$ and add the set $B_0=H^{\perp}$. We also define $$T_s:B_{m-1}\to B_{m}\setminus B_{m-1} \quad \text{by} \quad T_s(w)=w+s_0p^{-m},$$ so that $T_s$ maps $\Omega_{s,0}$ to $B_0(s)$ by translation. It is easy to verify that this data fit the requirements of [@Ben-Ben]: each $\Omega_{s,0}$ is $(\tau,{{\mathcal D}})$-congruent to $H^{\perp}=B_0$, the union of all such sets contains a neighborhood of $0$, each $T_s$ has the form required by formula [@Ben-Ben (4.1)], and for each $s\ne s'$ in $J_{p;m}$, one of the two compatibility condition [@Ben-Ben (4.2) or (4.3) ] holds. Thus, by using the algorithm of [@Ben-Ben], one can produce the wavelets (\[62.1\]). Moreover, according to (\[o-64.7\]), any wavelet $\theta_{s}^{(m)}$ is the Fourier transform


wavelets (\[62.0-1\]) are eigenfunctions of the one-dimensional fractional operator (\[61\*\*\]), (\[59\*\*\]) for $\alpha>0$: $$\label{62.2-v}
D^{\alpha}\theta_{k;\,j a}(x)=p^{\alpha(1-j)}\theta_{k;\,j a}(x),
\quad x\in {{\mathbb Q}}_p,$$ where $k=1,2,\dots p-1$,  $j\in {{\mathbb Z}}$, $a\in I_p$. Since wavelet functions (\[62.0-1\]) belong to the Lizorkin space, the relation (\[62.2-v\]) holds for all $\alpha\in {{\mathbb C}}$.

Now we study the spectral problem for pseudo-differential operators (\[64.3\]) in connection with the wavelet functions (\[62.8\]) and (\[62.8-1\]).

\[th4.1\] Let $A$ be a pseudo-differential operator [(\[64.3\])]{} with a symbol ${{\mathcal A}}(\xi)\in {{\mathcal E}}({{\mathbb Q}}_p^n\setminus \{0\})$. Then the $n$-dimensional non-Haar wavelet function [(\[62.8\])]{} $$\Theta_{s;\,j a}^{(m)\times}(x)=p^{-|j|/2}
\chi_p\big(s\cdot(\widehat{p^{j}}x-a)\big)
\Omega\big(|\widehat{p^{j}}x-a|_p\big), \quad x\in {{\mathbb Q}}_p^n,$$ is an eigenfunction of $A$ if and only if $$\label{64.1***}
{{\mathcal A}}\big(\widehat{p^{j}}(-s+\eta)\big)={{\mathcal A}}\big(-\widehat{p^{j}}s\big),
\qquad \forall \, \eta \in {{\mathbb Z}}_p^n,$$ where $j=(j_1,\dots,j_n)\in {{\mathbb Z}}^n$; $a\in I_p^n$; $s\in J_{p;m}^n$; and $m=(m_1,\dots,m_n)$, $m_j\ge 1$ is a [*fixed*]{} positive integer, $j=1,2,\dots,n$.string, Class. Quant. Grav. **4** (1987), L83–L87.

W. A. Zuniga-Galindo, Pseudo-differential equations connected with $p$-adic forms and local zeta functions, Bull. Austral. Math. Soc. **70** no. 1 (2004), 73–86.

W. A. Zuniga-Galindo, Fundamental solutions of pseudo-differential operators over $p$-adic fields, Rend. Sem. Mat. Univ. Padova **109** (2003), 241–245.

[^1]: Here we follow the referee report of the previous version of our paper.


O(n log n) for the sort plus time O(n) for the search (that could be reduced to O(n) if the items are integers

uh, it’s known that the sum of x from 1 to n is a formula: (n(n+1))/2, right? So, take the sum of your entire input array, subtract off the calculated constant, and you’re left with the duplicate value. No sorting or extra arrays necessary. :-)

@Mike: The integers in the array are not guaranteed to be from 1 to 1000000. They could be any value between 1 and 1000000, and you could have an arbitrary number of array elements. Your method would work otherwise :)

The logic is a mere two lines in racket. Unfortunately, this is assuming that no other integer appears more than once in thelevel.”

What began on election night as a sense of shock — Republicans recognized Barack Obama might win reelection, but few expected an Electoral College blowout — deepened into something more depressive on Wednesday as the sweep of the party’s defeat became clear.

Readers' Comments (784)

The republican philosophy of everything being state centric is wrong. The party itself feels that it cannot be state centric anymore and needs to be centralized. The same applies at the federal level too. You cannot have too small government and for gods sake please start come out of the foxland and for a moment start trusting the pollsters or atleast the trend of polls.

What we have to realize is that the USA is fast becoming a poor, third world nation demographically, dependent on massive


7:3" before attacking others.

Republicans must know and teach that We can't say "Right To Life while cutting food, raiment, shelter, Medical" because that's only saying, "Right To Just-Birth, then you are on your own." thus, the phrase becomes an Oxymoron.

Govenors inside The Republican Party Must Force The House of Representatives to "Stop Obstrution of Ideas that they know are both "Conservative and Republican" (ie Infrastructure, Personal Responsibility in HC-insurance)

Sidebar: [ Yes, it is harder than Gov McDonnell has begun to see; yet, he is positioned to impact this growth of truth in GOP Leadership. Mmmmmm, sorry Rep Eric Cantor is still stabbing Leader Boehner in the hip as he tries for a "Big 4 Trillion $$ Deal"]

Conservative Barry Goldwater warned about what would happen if the Republican partyThey then proceed to show how many more people are on welfare and food stamps over the past four years. They produce a bigoted idiot who swears what O'Really says is true.

The Republicans simply need to emulate the Democrats to right their political ship. Better (more honest and less politicized) pollsters, more computer and internet savvy and sophistication, and a real national ground game in place of the lazy psychological "enthusiasm" ruse.

Likewise, Republicans need to do as their leader did -- emulate the Democrat in attitude, ordering of values and policy prescriptions at home and abroad. Romney's last-minute desperate shadowing of President Obama in the debates gave him his only fleeting chance at victory. Still, we chose Obama over mini-Obama and for obvious reasons. But Republicans can solve


//
//  ImageDownloader.swift
//  Kingfisher
//
//  Created by Wei Wang on 15/4/6.
//
//  Copyright (c) 2016 Wei Wang <onevcat@gmail.com>
//
//  Permission is hereby granted, free of charge, to any person obtaining a copy
//  of this software and associated documentation files (the "Software"), to deal
//  in the Software without restriction, including without limitation the rights
//  to use, copy, modify, merge, publish, distribute, sublicense, and/or sell
//  copies of the Software, and to permit persons to whom the Software is
//  furnished to do so, subject to the following conditions:
//
//  The above copyright notice and this permission notice shall be included in
//  all copies or substantial portions of the Software.
//
//  THE SOFTWARE IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, EXPRESS OR
// var trustedHosts: Set<String>?

    /// Use this to set supply a configuration for the downloader. By default, NSURLSessionConfiguration.ephemeralSessionConfiguration() will be used.
    /// You could change the configuration before a downloaing task starts. A configuration without persistent storage for caches is requsted for downloader working correctly.
    open var sessionConfiguration = URLSessionConfiguration.ephemeral {
        didSet {
            session = URLSession(configuration: sessionConfiguration, delegate: sessionHandler, delegateQueue: OperationQueue.main)
        }
    }

    /// Whether the download requests should use pipeling or not. Default is false.
    open


Q:

how to terminate some process which is run with sudo with kill

with an unprivileged user account, using bash, I could do:
sudo /bin/sleep 6000

and kill it with Ctrl-c. However, sending SIGINT or SIGKILL from another terminal won't work for that purpose.
Anyone knows why is that? I'd like to be able to kill the process sending a signal, for using in a script, for example.
Regards.

A:

You're only allowed to send signals to a process running with the same UID (unless the sending process is running as root). When you use sudo, the new process is running as root, but if you try to kill it you're running as your normal userid. You would have to use sudo kill PID to kill it.
Signals sent from terminal control characters are treated specially: theyTeller's testament is the reactor accident in Pennsylvania at Three Mile Island in March 1979. As the nation panicked, Dr. Teller, an ardent backer of nuclear power, went on a public relations blitz to insist that the crisis was one of politics, not technology. In May 1979, he stressed the point to Congress.

The next day, Dr. Teller, then 71, suffered a heart attack.

"He called me from the intensive care unit," recalled Dr. George A. Keyworth II, a friend of Dr. Teller's at Los Alamos who later served as President Ronald Reagan's science adviser. He said the elder physicist began the call with two assertions: "Heart attacks are painful, and I have discovered that I am not immortal."

Dr. Keyworth recalled: "He was frightened, like a child."

Upon release from the


reply that is way too big. This is a thread to crash the server, so lets post a reply that is way too big. This is a thread to crash the server, so lets post a reply that is way too big. This is a thread to crash the server, so lets post a reply that is way too big. This is a thread to crash the server, so lets post a reply that is way too big. This is a thread to crash the server, so lets post a reply that is way too big. This is a thread to crash the server, so lets post a reply that is way too big. This is a thread to crash the server, so lets post a reply thatsince sliced white bread. Vasily Gatov, one of RIA’s most senior people, claimed that “Grozny” was afraid that the FBI would take the second Boston bomber alive (presumably, because the FSB trained him up, or something). Make no mistake, I do think that freedom of speech is good and it’s great that Eggert enjoys it in Russia – though it’s worth mentioning that the sentiment is not reciprocal – but the notion becomes rather absurd and even distorted when a state news agency consistently attacks and undermines the government in the eyes of foreigners.

This does not happen in the West. Whatever their domestic disagreements, there is an implicit understanding among American politicians that criticism of the US and the US government is off limits so far as foreigners


I was told privately the other (Russian) columnists had complained that “this foreigner” works too hard and makes us all look bad. Then RT (then Russia Today) came along. This is an entirely different story (and will wait for later). Two remaining things stay with me about RIA. First, they wouldn’t let me quit! No, I would have to stay, even if I didn’t write for them I stayed and would be paid. That lasted for about six months. I don’t recall collecting my wages from them in remaining months; it was so idiotic. Second, as RT expanded (literally in the RIA building), RT staff was treated like second-class citizens. Our ability to move about the building was at times bordering on the ridiculous. In the end weis now most deeply rooted in the Internet.

A rationalization of this unwieldy mess of Soviet-era legacy organizations is well past due, and that is seemingly what is going to happen. RIA, Voice of Russia, and RBTH will all be consolidated into Russia Segodnya. RT will remain separate.

There are difficulties and unresolved issues. For instance, RIA itself has a vast and rather disorganized number of projects, such as RAPSI (provides legal information, esp. on trials and sucklike), Valdai (meetings of foreign and Russian experts to discuss Russia’s trajectory, culminating in yearly meetings with Putin), and InoSMI (a resource that translates foreign media into Russian). Many of these projects are genuinely useful, and while RIA itself may be superfluous, I very much hope that they will continue either under Rossiya


Over the past few weeks, we’ve heard more and more about different modes for Switch when it’s docked and when the device is being played as a standalone unit. That culminated with a report from Digital Foundry just a couple of days ago. The publication claims that Switch, when in portable mode, runs at 40 percent of the clock-speed of the fully docked device.

Unreal Engine 4 version 4.14 released about a month ago. One developer has now come across some interesting discoveries which lend credence to some of the recent speculation.

A file in Unreal Engine 4’s master branch shows names for Switch, SwitchConsole and SwitchHandheld. As the developer points out, “the SwitchConsole settings are a notch lower than the UE4 defaults used on PC, PS4 and XB1.” It’s[SwitchConsole DeviceProfile]

DeviceType=Switch

BaseProfileName=Switch [SwitchHandheld DeviceProfile]

DeviceType=Switch

BaseProfileName=Switch

+CVars=sg.ViewDistanceQuality=1

+CVars=sg.AntiAliasingQuality=1

+CVars=sg.ShadowQuality=1

+CVars=sg.PostProcessQuality=1

+CVars=sg.TextureQuality=1

+CVars=sg.EffectsQuality=1

+CVars=r.ScreenPercentage=66

There’s still a lot that’s unclear, but this helps to fill in a piece of the puzzle. Nintendo will hopefully fully explain how Switch works when docked and playing as a handheld during its big unveiling event next month.

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the License for the specific language governing permissions and
   limitations under the License.

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package org.apache.batik.css.engine.sac;

import org.w3c.dom.Element;

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