{"id":12287,"date":"2023-05-28T14:37:23","date_gmt":"2023-05-28T11:37:23","guid":{"rendered":"https:\/\/bestessayhomework.com\/tr\/?p=12287"},"modified":"2023-05-28T14:37:23","modified_gmt":"2023-05-28T11:37:23","slug":"atif-kullanim-sinirlamalari","status":"publish","type":"post","link":"https:\/\/bestessayhomework.com\/tr\/atif-kullanim-sinirlamalari\/","title":{"rendered":"At\u0131f Kullan\u0131m S\u0131n\u0131rlamalar\u0131"},"content":{"rendered":"

At\u0131f Kullan\u0131m S\u0131n\u0131rlamalar\u0131<\/span><\/strong><\/h3>\n

At\u0131f da\u011f\u0131l\u0131mlar\u0131n\u0131n dura\u011fan olmayan do\u011fas\u0131 zaten fark edilmi\u015fti. Fizik makalelerinin at\u0131f \u00f6mr\u00fcn\u00fcn, at\u0131f say\u0131s\u0131yla artt\u0131\u011f\u0131 bulundu. Makalelerin kesirleriyle tan\u0131mland\u0131\u011f\u0131 \u015fekliyle y\u00fcksek enerjili fizik makalelerinin \u00f6mr\u00fcn\u00fc analiz etti ve ayr\u0131ca \u00f6mr\u00fcn al\u0131nt\u0131 say\u0131s\u0131yla artt\u0131\u011f\u0131n\u0131 buldu.<\/span><\/p>\n

Y\u00fcksek at\u0131f yap\u0131lan makalelerin at\u0131f y\u00f6r\u00fcngelerinin niteliksel olarak di\u011ferlerinden farkl\u0131 oldu\u011funu ve doygunlu\u011fa ula\u015fmad\u0131\u011f\u0131n\u0131 g\u00f6sterdi. Olu\u015fturulan yo\u011funla\u015ft\u0131rma yasas\u0131, zaman ge\u00e7tik\u00e7e b\u00fcy\u00fcyen al\u0131nt\u0131 a\u011flar\u0131n\u0131n kendi kendine benzer olmad\u0131\u011f\u0131n\u0131, \u00e7ap\u0131n\u0131n k\u00fc\u00e7\u00fcld\u00fc\u011f\u00fcn\u00fc ve daha yo\u011fun hale geldi\u011fini belirtir.<\/span><\/p>\n

A\u015fa\u011f\u0131da, bu \u015fa\u015f\u0131rt\u0131c\u0131 dura\u011fan olmaman\u0131n a\u00e7\u0131klamas\u0131n\u0131 buluyoruz. Her \u015feyden \u00f6nce, dura\u011fan olmayan uzun at\u0131f \u00f6mr\u00fcn\u00fcn \u00f6nemsiz bir kayna\u011f\u0131 vard\u0131r. Ger\u00e7ekten de \u00f6l\u00e7\u00fcmlerimiz, s\u0131radan Fizik, Ekonomi ve Matematik makalelerinin karakteristik at\u0131f \u00f6mr\u00fcn\u00fcn s\u0131ras\u0131yla \u03c40 = 4,6,9 ve 11,8 y\u0131l oldu\u011funu g\u00f6stermektedir.<\/span><\/p>\n

\u00dcstel s\u00fcre\u00e7, \u223c3\u03c40’dan sonra doyuma ula\u015f\u0131r. Bu nedenle, diyelim ki 15 y\u0131ll\u0131k zaman penceresini d\u00fc\u015f\u00fcn\u00fcrsek, s\u0131radan Fizik makaleleri i\u00e7in at\u0131f da\u011f\u0131l\u0131mlar\u0131 zaten dura\u011fan olmal\u0131, Ekonomi ve Matematik i\u00e7in olanlar ise hen\u00fcz dura\u011fan de\u011fil.<\/span><\/p>\n

Pek \u00e7ok at\u0131f da\u011f\u0131l\u0131m\u0131, s\u0131radan makalelerin bile at\u0131f kariyerinin tamamlanmad\u0131\u011f\u0131, yay\u0131nland\u0131ktan sonraki sadece 5-10 y\u0131ll\u0131k zaman aral\u0131\u011f\u0131nda \u00f6l\u00e7\u00fclm\u00fc\u015ft\u00fcr, dolay\u0131s\u0131yla bu t\u00fcr da\u011f\u0131l\u0131mlar\u0131n dura\u011fan olmamas\u0131 ve farkl\u0131 \u015fekiller sergilemesi \u015fa\u015f\u0131rt\u0131c\u0131 de\u011fildir.<\/span><\/p>\n

Dura\u011fan olmaman\u0131n daha \u00f6nemli bir kayna\u011f\u0131, bir makalenin at\u0131f s\u00fcresinin at\u0131f say\u0131s\u0131yla artmas\u0131d\u0131r ve bu durum incelenen t\u00fcm ara\u015ft\u0131rma alanlar\u0131 i\u00e7in ge\u00e7erlidir. Bu say\u0131, her alan ve yay\u0131n y\u0131l\u0131 i\u00e7in belirli bir Kr kritik say\u0131s\u0131n\u0131 a\u015ft\u0131\u011f\u0131nda, at\u0131f \u00f6mr\u00fc sonsuza kadar gider, \u00f6yle ki K > Kr olan makaleler ka\u00e7ak veya s\u00fcper kritik makaleler haline gelir.<\/span><\/p>\n

Kontrolden \u00e7\u0131kma davran\u0131\u015f\u0131n\u0131n kayna\u011f\u0131n\u0131 kopyalama\/yinelemeli arama mekanizmam\u0131z \u00e7er\u00e7evesinde a\u00e7\u0131kl\u0131yoruz. Ger\u00e7ekten de, yeni yay\u0131nlanan her makale, yazarlar\u0131n\u0131n veritabanlar\u0131nda, \u0130nternet’te vb. buldu\u011fu bir dizi makaleye at\u0131fta bulunur.<\/span><\/p>\n

Bu at\u0131f makalelerinin her biri, yazarlar\u0131n\u0131n kaynak makaleyi referans listelerine kopyalayabilecekleri bir ikincil at\u0131f makaleleri dizisini tetikler. Bu kademenin azal\u0131p azalmad\u0131\u011f\u0131 veya yay\u0131ld\u0131\u011f\u0131\u2014bu, Rr ep = P0 N nn yeniden \u00fcretim say\u0131s\u0131na ba\u011fl\u0131d\u0131r; burada N nn, bir birinci nesil at\u0131f makalesi ba\u015f\u0131na ikinci nesil at\u0131f makalelerinin ortalama say\u0131s\u0131d\u0131r (yay\u0131lma katsay\u0131s\u0131) ve P0, dolayl\u0131 al\u0131nt\u0131 yapma (kopyalama) olas\u0131l\u0131\u011f\u0131d\u0131r.<\/span><\/p>\n

S\u0131radan makaleler i\u00e7in Rrep < 1 ve at\u0131f kaskad\u0131 azal\u0131rken, \u00e7ok at\u0131f yap\u0131lan makaleler i\u00e7in Rrep > 1 ve at\u0131f kaskad\u0131 zaman i\u00e7inde s\u00fcresiz olarak yay\u0131l\u0131r. Rrep = 1 olan devrilme noktas\u0131n\u0131n \u00fcstesinden gelmeyi ba\u015faran ka\u011f\u0131tlar ka\u00e7akt\u0131r ve varl\u0131klar\u0131 “kazanan her \u015feyi al\u0131r” a\u011f\u0131na neden olabilir.<\/span><\/p>\n

Derece da\u011f\u0131l\u0131m\u0131na g\u00f6re at\u0131f a\u011f\u0131n\u0131n dura\u011fan olmamas\u0131n\u0131n sonu\u00e7lar\u0131 nelerdir? Bir y\u0131l i\u00e7inde bir alanda yay\u0131nlanm\u0131\u015f makale grubuna odaklan\u0131rsak, ilk zamanlarda at\u0131f da\u011f\u0131l\u0131m\u0131 uygunluk da\u011f\u0131l\u0131m\u0131n\u0131 taklit ederken, daha sonraki zamanlarda modelimize g\u00f6re geli\u015fir.<\/span><\/p>\n

\u0130lk at\u0131f da\u011f\u0131l\u0131m\u0131 log-normal’e yak\u0131nken, geli\u015fen da\u011f\u0131l\u0131mlar d\u00fczle\u015fir ve kuvvet yasas\u0131na daha yak\u0131n hale gelir. Bu, g\u00fc\u00e7 yasas\u0131 derecesi da\u011f\u0131l\u0131m\u0131n\u0131n yaln\u0131zca statik a\u011flarda, yani uzun bir geli\u015fim s\u00fcrecinden ge\u00e7mi\u015f a\u011flarda bulunabilece\u011fini varsayanlar\u0131n tahminini do\u011frular. Burada, bir zamanlar statik olarak kabul edilen uzun zaman s\u0131n\u0131r\u0131ndaki at\u0131f da\u011f\u0131l\u0131m\u0131n\u0131n asl\u0131nda her zaman ge\u00e7ici oldu\u011funu g\u00f6steriyoruz.<\/span><\/p>\n

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Al\u0131nt\u0131 ve at\u0131f<\/a> aras\u0131ndaki fark<\/span>
\nMakale i\u00e7indeki al\u0131nt\u0131dan al\u0131nt\u0131 yapma APA<\/span>
\nDo\u011frudan al\u0131nt\u0131 \u00f6rne\u011fi<\/span>
\nKanun kaynak\u00e7ada nas\u0131l g\u00f6sterilir APA<\/span>
\nMetin i\u00e7inde kaynak G\u00f6sterme<\/span>
\nDolayl\u0131 al\u0131nt\u0131 nas\u0131l yap\u0131l\u0131r<\/span>
\nAPA 7 aktaran G\u00f6sterme<\/span>
\nAt\u0131f yapmak Ne Demek<\/span><\/p>\n

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Zaman ge\u00e7tik\u00e7e kuyru\u011fu d\u0131\u015fb\u00fckeyden d\u00fcz \u00e7izgiye evrilir ve daha sonra i\u00e7b\u00fckey \u015fekli bile alabilir. Bu evrimin h\u0131z\u0131 alana \u00f6zg\u00fcd\u00fcr ve uygunluk da\u011f\u0131l\u0131m\u0131na, bu alandaki yay\u0131n say\u0131s\u0131ndaki art\u0131\u015fa ve ortalama referans listesi uzunlu\u011funa ba\u011fl\u0131d\u0131r.<\/span><\/p>\n

Peki, \u201cg\u00fc\u00e7 kanunu\u201d at\u0131f da\u011f\u0131l\u0131mlar\u0131n\u0131n kayna\u011f\u0131 nedir? Bulgular\u0131m\u0131z, bunlar\u0131n uygunluk da\u011f\u0131l\u0131m\u0131ndan miras al\u0131nd\u0131\u011f\u0131n\u0131 ve daha sonra al\u0131nt\u0131 i\u015flemi s\u0131ras\u0131nda de\u011fi\u015ftirildi\u011fini g\u00f6stermektedir. At\u0131f da\u011f\u0131l\u0131mlar\u0131n\u0131n neden kuvvet yasas\u0131 ba\u011f\u0131ml\u0131l\u0131\u011f\u0131n\u0131 takip etti\u011fi sorusu bu nedenle uygunluk da\u011f\u0131l\u0131m\u0131na indirgenir. Derin soru, uygunluk da\u011f\u0131l\u0131m\u0131n\u0131n neden belirli bir \u015fekle sahip oldu\u011fu ve bu \u015feklin evrensel g\u00f6r\u00fcnd\u00fc\u011f\u00fcd\u00fcr.<\/span><\/p>\n

G\u00fc\u00e7 yasas\u0131 derecesi da\u011f\u0131l\u0131m\u0131 mutlaka \u00f6l\u00e7eksiz bir a\u011f anlam\u0131na m\u0131 geliyor? \u00d6l\u00e7ekten ba\u011f\u0131ms\u0131z a\u011flar kavram\u0131, karma\u015f\u0131k a\u011flarda g\u00fc\u00e7 yasas\u0131 derece da\u011f\u0131l\u0131mlar\u0131n\u0131n her yerde bulunmas\u0131n\u0131n baz\u0131 evrensel \u00fcretici mekanizmalara i\u015faret etti\u011fini fark edenler taraf\u0131ndan tan\u0131t\u0131ld\u0131.<\/span><\/p>\n

Barabasi-Albert tercihli ba\u011flanma mekanizmas\u0131, uzun zaman s\u0131n\u0131r\u0131nda derece da\u011f\u0131l\u0131m\u0131 dura\u011fan hale gelen, b\u00fcy\u00fcyen karma\u015f\u0131k bir a\u011f olu\u015fturur. Bu dura\u011fan \u015fekil, \u00f6l\u00e7eksiz a\u011f\u0131 ima eden g\u00fc\u00e7 yasas\u0131d\u0131r.<\/span><\/p>\n

Karma\u015f\u0131k a\u011flar\u0131n ortaya \u00e7\u0131kmas\u0131ndan \u00f6nce, \u00f6l\u00e7eksiz olgular yo\u011fun madde fizi\u011finde ortaya \u00e7\u0131kt\u0131 ve genellikle faz ge\u00e7i\u015fleri ve kritik noktalarla ili\u015fkilendirildi. Yo\u011fun madde fizi\u011finde, bu fenomen korelasyon uzunlu\u011fu ile ili\u015fkili karakteristik \u00f6l\u00e7ek, kritik noktada farkl\u0131la\u015f\u0131r ve bu, maddenin statik ve dinamik \u00f6zellikleri i\u00e7in evrensel g\u00fc\u00e7 yasalar\u0131yla sonu\u00e7lan\u0131r.<\/span><\/p>\n

Karma\u015f\u0131k a\u011flardaki evrensel g\u00fc\u00e7 yasas\u0131 derecesi da\u011f\u0131l\u0131m\u0131, b\u00fcy\u00fck birle\u015fik teoriler aray\u0131\u015f\u0131ndaki fizik\u00e7iler i\u00e7in b\u00fcy\u00fck bir \u00e7ekicili\u011fe sahiptir, \u00e7\u00fcnk\u00fc bu t\u00fcr \u00e7e\u015fitli nesnelerin, karma\u015f\u0131k a\u011flar\u0131n ve kritik noktadaki maddelerin \u00f6zelliklerinin ayn\u0131 matematiksel bi\u00e7imcilik taraf\u0131ndan tan\u0131mland\u0131\u011f\u0131n\u0131 ima eder.<\/span><\/p>\n

Bununla birlikte, kuvvet yasas\u0131 derece da\u011f\u0131l\u0131m\u0131 ile karma\u015f\u0131k bir a\u011f\u0131n \u00f6l\u00e7eksiz karakteri aras\u0131ndaki denklik, yaln\u0131zca derece da\u011f\u0131l\u0131m\u0131 dura\u011fansa veya en az\u0131ndan \u015feklini de\u011fi\u015ftirmiyorsa ge\u00e7erlidir. Ancak, dura\u011fan olmayan a\u011flar i\u00e7in a\u011f geli\u015fimini y\u00f6neten dinamik bir \u00f6l\u00e7ek olabilir.<\/span><\/p>\n

Burada al\u0131nt\u0131 da\u011f\u0131l\u0131mlar\u0131n\u0131n dura\u011fan olmad\u0131\u011f\u0131n\u0131, \u015fekillerinin zamanla de\u011fi\u015fti\u011fini ve a\u011f b\u00fcy\u00fcmesi i\u00e7in \u00f6nemli olan belirli bir dinamik \u00f6l\u00e7ek oldu\u011funu g\u00f6steriyoruz. Bu nedenle, karma\u015f\u0131k bir a\u011f, derece da\u011f\u0131l\u0131m\u0131 bir g\u00fc\u00e7 yasas\u0131 ba\u011f\u0131ml\u0131l\u0131\u011f\u0131n\u0131 takip etse bile \u00f6l\u00e7eksiz olmayabilir.<\/span><\/p>\n

Bulgular\u0131m\u0131z di\u011fer karma\u015f\u0131k a\u011flara geni\u015fletilebilir mi? Dura\u011fan olmayan at\u0131f da\u011f\u0131l\u0131m\u0131n\u0131n do\u011frusal olmayan at\u0131f dinamikleri ile ili\u015fkili oldu\u011funu bulduk. Patentlerin al\u0131nt\u0131 dinamikleri de do\u011frusal de\u011fildir.<\/span><\/p>\n

Bu nedenle, patent at\u0131f da\u011f\u0131l\u0131m\u0131n\u0131n da dura\u011fan olmamas\u0131n\u0131 bekliyoruz. \u0130nternet a\u011flar\u0131ndaki derece da\u011f\u0131l\u0131m\u0131 ile ilgili olarak – ikincisinin \u00f6nemli bir fark\u0131 vard\u0131r: y\u00f6nlendirilmi\u015f ve d\u00f6ng\u00fcsel olmayan al\u0131nt\u0131 a\u011flar\u0131n\u0131n aksine, WWW de\u011fildir ve oradaki ba\u011flant\u0131lar d\u00fczenlenebilir. Bununla birlikte, Web sayfas\u0131 pop\u00fclaritesinin da\u011f\u0131l\u0131m\u0131nda da ka\u00e7aklar tespit edildi.<\/span><\/p>\n

\u00d6zetle, bilimsel makalelere yap\u0131lan at\u0131flar\u0131n istatistiki da\u011f\u0131l\u0131m\u0131n\u0131n kuvvet-kural ba\u011f\u0131ml\u0131l\u0131\u011f\u0131na uydurulabilirken, bu da\u011f\u0131l\u0131m\u0131n dura\u011fan olmad\u0131\u011f\u0131n\u0131 ve uzun zaman diliminde s\u0131n\u0131rlay\u0131c\u0131 bir \u015fekil almad\u0131\u011f\u0131n\u0131 g\u00f6sterdik.<\/span><\/p>\n

G\u00fc\u00e7 kanunu uyumu, \u00f6l\u00e7ekten ba\u011f\u0131ms\u0131z at\u0131f a\u011f\u0131n\u0131 ima ederken, ka\u00e7aklar\u0131n ba\u015flang\u0131c\u0131yla ili\u015fkili gizli bir dinamik \u00f6l\u00e7ek oldu\u011funu g\u00f6steriyoruz. Bu nedenle, \u00f6l\u00e7\u00fclen at\u0131f da\u011f\u0131l\u0131mlar\u0131 ile g\u00fc\u00e7 yasas\u0131 ba\u011f\u0131ml\u0131l\u0131\u011f\u0131 aras\u0131ndaki benzerli\u011fin derin etkileri yoktur.<\/span><\/p>\n

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