| The entire DSpace / Artikkelit / TUHAT-tuplat (temp) | 1 / 2023 | 2 / 2023 | 3 / 2023 | 4 / 2023 | 5 / 2023 | 6 / 2023 | 7 / 2023 | 8 / 2023 | 9 / 2023 | 10 / 2023 | 11 / 2023 | 12 / 2023 | Total |
|---|
| 'Simultaneously impressed with one delusion' | 3 |
2 |
4 |
2 |
4 |
0 |
0 |
0 |
2 |
0 |
0 |
2 |
19 |
| A Hub Architecture For Service Ecosystems: Towards Business-to-Business Automation with an Ontology-Enabled Collaboration Platform | 3 |
1 |
7 |
9 |
7 |
11 |
0 |
0 |
1 |
0 |
2 |
0 |
41 |
| Alignment of the CMS Silicon Tracker during Commissioning with Cosmic Rays | 3 |
2 |
2 |
3 |
5 |
5 |
0 |
1 |
4 |
3 |
0 |
0 |
28 |
| Approximate string matching with reduced alphabet | 16 |
5 |
10 |
6 |
11 |
8 |
0 |
1 |
2 |
0 |
1 |
1 |
61 |
| Balancing the needs of capercaillie (Tetrao urogallus) and moose (Alces alces) in large-scale human land use | 6 |
5 |
3 |
2 |
8 |
4 |
0 |
1 |
2 |
0 |
0 |
2 |
33 |
| Biocompatibility of Thermally Hydrocarbonized Porous Silicon Nanoparticles and their Biodistribution in Rats | 23 |
18 |
19 |
22 |
12 |
15 |
2 |
4 |
1 |
6 |
9 |
2 |
133 |
| Bit-parallel search algorithms for long patterns | 8 |
7 |
9 |
7 |
12 |
9 |
0 |
2 |
3 |
3 |
2 |
2 |
64 |
| Bryophyte flora of Hunan Province, China. 10. Ulota gymnostoma sp nova (Orthotrichaceae) | 7 |
1 |
1 |
1 |
3 |
1 |
0 |
1 |
1 |
1 |
1 |
1 |
19 |
| Bryophyte flora of Hunan Province, China. 10. Ulota gymnostoma sp nova (Orthotrichaceae) | 2 |
1 |
2 |
4 |
5 |
1 |
0 |
0 |
1 |
2 |
1 |
0 |
19 |
| Classifiers for educational technology | 4 |
1 |
7 |
9 |
16 |
15 |
0 |
3 |
1 |
1 |
1 |
2 |
60 |
| CMS Data Processing Workflows during an Extended Cosmic Ray Run | 8 |
3 |
4 |
1 |
4 |
3 |
0 |
0 |
1 |
0 |
0 |
0 |
24 |
| Collecting data from distributed FOSS projects | 2 |
2 |
1 |
0 |
5 |
1 |
0 |
1 |
2 |
0 |
1 |
0 |
15 |
| Commissioning and Performance of the CMS Silicon Strip Tracker with Cosmic Ray Muons | 7 |
4 |
2 |
2 |
4 |
3 |
0 |
1 |
1 |
0 |
3 |
0 |
27 |
| Comparisons by Location and Gender | 4 |
1 |
4 |
5 |
13 |
7 |
2 |
2 |
2 |
0 |
0 |
1 |
41 |
| Comparisons by Location and Gender | 4 |
4 |
11 |
4 |
6 |
9 |
0 |
6 |
3 |
1 |
8 |
6 |
62 |
| compatibility with a hybrid GO model | 2 |
0 |
5 |
4 |
6 |
5 |
1 |
1 |
4 |
0 |
0 |
1 |
29 |
| Effect of the Calibration in Water and the Build-up Cap on the Mg(Ar) Ionization Chamber Measurements | 10 |
1 |
3 |
2 |
4 |
5 |
1 |
1 |
1 |
3 |
2 |
2 |
35 |
| Effect of the Calibration in Water and the Build-up Cap on the Mg(Ar) Ionization Chamber Measurements | 6 |
3 |
4 |
1 |
6 |
2 |
1 |
2 |
4 |
3 |
4 |
3 |
39 |
| Espoo shootings: A failure of restraint | 0 |
1 |
7 |
5 |
4 |
3 |
0 |
0 |
0 |
1 |
0 |
0 |
21 |
| Europeanisation and Compensating Harms Caused by Competition Restrictions | 9 |
6 |
5 |
2 |
4 |
6 |
1 |
3 |
1 |
0 |
1 |
1 |
39 |
| Evaluation of the SAF AIS implementations | 9 |
2 |
2 |
1 |
5 |
3 |
0 |
3 |
2 |
3 |
1 |
0 |
31 |
| Finnish CMS-TOB cosmic rack | 9 |
5 |
3 |
8 |
6 |
6 |
2 |
2 |
3 |
0 |
0 |
0 |
44 |
| First Measurement of the Ratio of Branching Fractions B(Lambda_b to Lambda_c mu nu)/B(Lambda_b to Lambda_c pi) | 6 |
3 |
320 |
3 |
1 |
3 |
0 |
0 |
1 |
0 |
0 |
1 |
338 |
| First Observation of B̅ s0→Ds±K∓ and Measurement of the Ratio of Branching Fractions B(B̅ s0→Ds±K∓)/B(B̅ s0→Ds+π-) | 5 |
5 |
492 |
175 |
4 |
5 |
0 |
0 |
1 |
0 |
1 |
0 |
688 |
| First observation of the decay Bs --> Ds K and measurement of the ratio of branching fractions Br(Bs --> DsK)/Br(Bs --> Ds pi) | 6 |
5 |
322 |
9 |
1 |
4 |
0 |
0 |
1 |
0 |
1 |
0 |
349 |
| First Observation of Vector Boson Pairs in a Hadronic Final State at the Tevatron Collider | 5 |
9 |
491 |
181 |
2 |
6 |
0 |
0 |
0 |
0 |
1 |
0 |
695 |
| How can mobile production promote pupils in portfolio-work in language learning | 2 |
3 |
8 |
5 |
5 |
7 |
2 |
1 |
1 |
1 |
1 |
0 |
36 |
| Ideal tau tagging with the multivariate data-analysis toolkit TMVA | 8 |
2 |
4 |
0 |
4 |
2 |
0 |
0 |
2 |
0 |
1 |
1 |
24 |
| Identification and Filtering of Uncharacteristic Noise in the CMS Hadron Calorimeter | 4 |
3 |
5 |
1 |
3 |
5 |
0 |
0 |
2 |
0 |
1 |
4 |
28 |
| Identification and Filtering of Uncharacteristic Noise in the CMS Hadron Calorimeter | 4 |
2 |
2 |
3 |
3 |
4 |
1 |
0 |
2 |
0 |
0 |
0 |
21 |
| Implications of Bohmian quantum ontology for psychopathology | 4 |
6 |
5 |
17 |
12 |
12 |
0 |
1 |
2 |
2 |
1 |
0 |
62 |
| Ion irradiation of multi-walled boron nitride nanotubes | 11 |
5 |
6 |
7 |
6 |
8 |
0 |
3 |
2 |
2 |
1 |
2 |
53 |
| Itseriittoisuus on aina vastenmielistä | 4 |
3 |
0 |
2 |
2 |
5 |
0 |
0 |
2 |
0 |
0 |
0 |
18 |
| Itseriittoisuus on aina vastenmielistä | 0 |
3 |
3 |
0 |
1 |
1 |
0 |
1 |
0 |
1 |
1 |
0 |
11 |
| Magnetically Induced Currents in [n]Cycloparaphenylenes, n=6-11 | 8 |
3 |
5 |
10 |
9 |
7 |
0 |
2 |
4 |
2 |
1 |
2 |
53 |
| Magnetically Induced Currents in [n]Cycloparaphenylenes, n=6-11 | 5 |
0 |
4 |
2 |
3 |
5 |
0 |
1 |
2 |
2 |
3 |
3 |
30 |
| Making multi-dimensional trust decisions on inter-enterprise collaborations | 10 |
5 |
5 |
11 |
7 |
13 |
0 |
2 |
1 |
2 |
0 |
0 |
56 |
| Measurement of Particle Production and Inclusive Differential Cross Sections in pbar{p} Collisions at sqrt{s}=1.96 TeV | 1 |
1 |
4 |
2 |
4 |
3 |
0 |
0 |
1 |
1 |
0 |
0 |
17 |
| Measurement of the b-hadron production cross section using decays to μ-D0X final states in pp̅ collisions at √s=1.96 TeV | 6 |
6 |
495 |
16 |
3 |
6 |
0 |
1 |
1 |
2 |
1 |
1 |
538 |
| Measurement of the b-hadron production cross section using decays to μ-D0X final states in pp̅ collisions at √s=1.96 TeV | 5 |
7 |
490 |
184 |
3 |
5 |
0 |
0 |
0 |
1 |
0 |
0 |
695 |
| Measurement of the kT Distribution of Particles in Jets Produced in pp̅ Collisions at √s=1.96 TeV | 7 |
5 |
496 |
174 |
4 |
4 |
0 |
0 |
1 |
1 |
1 |
0 |
693 |
| Measurement of the Ratio σtt̅ /σZ/γ*→ll and Precise Extraction of the tt̅ Cross Section | 6 |
6 |
494 |
172 |
2 |
5 |
0 |
0 |
4 |
0 |
0 |
3 |
692 |
| Measurement of the Ratio σtt̅ /σZ/γ*→ll and Precise Extraction of the tt̅ Cross Section | 6 |
5 |
495 |
8 |
3 |
6 |
0 |
0 |
2 |
0 |
0 |
1 |
526 |
| Measurement of the Single Top Quark Production Cross Section at CDF | 6 |
2 |
319 |
2 |
3 |
3 |
0 |
1 |
0 |
1 |
0 |
0 |
337 |
| Measurement of the top quark mass in the dilepton channel using mT2 at CDF | 3 |
3 |
5 |
3 |
1 |
2 |
0 |
0 |
1 |
1 |
1 |
0 |
20 |
| Measurement of the top quark mass with dilepton events selected using neuroevolution at CDF | 8 |
4 |
321 |
5 |
1 |
2 |
0 |
0 |
2 |
5 |
1 |
1 |
350 |
| Measurement of the tt̅ production cross section in 2 fb-1 of pp̅ collisions at √s=1.96 TeV using lepton plus jets events with soft muon b tagging | 5 |
8 |
496 |
18 |
3 |
5 |
0 |
0 |
2 |
0 |
1 |
0 |
538 |
| Measurement of the tt̅ production cross section in 2 fb-1 of pp̅ collisions at √s=1.96 TeV using lepton plus jets events with soft muon b tagging | 5 |
5 |
498 |
182 |
3 |
4 |
0 |
1 |
3 |
0 |
2 |
2 |
705 |
| Measurements of the top-quark mass using charged particle tracking | 8 |
2 |
627 |
3 |
2 |
3 |
0 |
0 |
1 |
0 |
0 |
0 |
646 |
| Multiple aspects of validity theory in the service of an oral proficiency assessment project | 1 |
4 |
8 |
5 |
3 |
6 |
0 |
3 |
0 |
0 |
2 |
0 |
32 |
| Neckera xizangensis (Neckeraceae, Bryophyta), a new species from China | 8 |
2 |
8 |
33 |
10 |
3 |
0 |
0 |
1 |
2 |
0 |
1 |
68 |
| Neckera xizangensis (Neckeraceae, Bryophyta), a new species from China | 15 |
2 |
5 |
1 |
3 |
5 |
0 |
0 |
1 |
1 |
2 |
1 |
36 |
| Observation of exclusive charmonium production and gamma+gamma to mu+mu- in p+pbar collisions at sqrt{s} = 1.96 TeV | 6 |
3 |
3 |
10 |
1 |
2 |
0 |
0 |
0 |
1 |
0 |
0 |
26 |
| Observation of exclusive charmonium production and gamma+gamma to mu+mu- in p+pbar collisions at sqrt{s} = 1.96 TeV | 4 |
1 |
3 |
7 |
2 |
2 |
0 |
0 |
1 |
0 |
0 |
0 |
20 |
| Observation of single top quark production and measurement of |Vtb| with CDF | 28 |
6 |
493 |
181 |
6 |
4 |
0 |
0 |
1 |
1 |
1 |
0 |
721 |
| On the consistency of sequentially normalized least squares | 8 |
5 |
2 |
3 |
5 |
4 |
1 |
1 |
3 |
0 |
0 |
0 |
32 |
| On the consistency of sequentially normalized least squares | 4 |
3 |
3 |
1 |
3 |
4 |
0 |
0 |
1 |
1 |
0 |
0 |
20 |
| Oswald Ducrot, Ranskan Monsieur Argumentation | 1 |
2 |
2 |
1 |
6 |
0 |
0 |
1 |
1 |
0 |
0 |
0 |
14 |
| Performance of CMS Muon Reconstruction in Cosmic-Ray Events | 1 |
3 |
3 |
1 |
3 |
3 |
0 |
1 |
2 |
2 |
2 |
2 |
23 |
| Popkritiikki leijonankesytyksenä | 4 |
4 |
4 |
2 |
2 |
5 |
0 |
0 |
0 |
0 |
0 |
0 |
21 |
| Popkritiikki leijonankesytyksenä | 4 |
4 |
2 |
3 |
4 |
9 |
0 |
0 |
1 |
0 |
0 |
0 |
27 |
| Production of psi(2S) Mesons in ppbar Collisions at 1.96 TeV | 8 |
3 |
703 |
4 |
3 |
2 |
0 |
0 |
1 |
0 |
0 |
0 |
724 |
| Re-evaluation of Rapakivi Petrogenesis: Source Constraints from the Hf Isotope Composition of Zircon in the Rapakivi Granites and Associated Mafic Rocks of Southern Finland | 5 |
6 |
6 |
9 |
6 |
5 |
0 |
1 |
3 |
0 |
2 |
5 |
48 |
| Search for a Fermiophobic Higgs Boson Decaying into Diphotons in p p-bar Collisions at sqrt{s} = 1.96 TeV | 3 |
5 |
3 |
9 |
1 |
2 |
0 |
0 |
0 |
1 |
0 |
0 |
24 |
| Search for Bs0→μ+μ- and B0→μ+μ- Decays with 2 fb-1 of pp̅ Collisions | 9 |
8 |
499 |
182 |
3 |
5 |
0 |
1 |
2 |
0 |
0 |
0 |
709 |
| Search for exclusive Z boson production and observation of high mass ppbar->gammagamma->p+ll+pbar events in ppbar collisions at sqrt(s) = 1.96 TeV | 9 |
4 |
4 |
2 |
1 |
2 |
0 |
0 |
1 |
0 |
1 |
2 |
26 |
| Search for Higgs bosons predicted in two-Higgs-doublet models via decays to tau lepton pairs in 1.96 TeV proton-antiproton collisions | 5 |
3 |
4 |
2 |
3 |
3 |
0 |
1 |
1 |
2 |
2 |
0 |
26 |
| Search for New Bottomlike Quark Pair Decays QQ̅ →(tW∓)(t̅ W±) in Same-Charge Dilepton Events | 5 |
8 |
491 |
176 |
3 |
4 |
0 |
0 |
1 |
0 |
2 |
1 |
691 |
| Search for the associated production of the standard-model Higgs boson in the all-hadronic channel | 5 |
3 |
325 |
10 |
2 |
2 |
0 |
0 |
0 |
0 |
0 |
0 |
347 |
| Search for the rare decays B+→μ+μ-K+, B0→μ+μ-K*(892)0, and Bs0→μ+μ-ϕ at CDF | 6 |
8 |
490 |
182 |
4 |
4 |
0 |
0 |
1 |
0 |
1 |
0 |
696 |
| Search for WW and WZ Resonances Decaying to Electron, Missing ET, and Two Jets in pp̅ Collisions at √s=1.96 TeV. | 5 |
6 |
489 |
174 |
3 |
5 |
0 |
0 |
1 |
0 |
0 |
0 |
683 |
| SiD Letter of Intent | 5 |
0 |
711 |
1 |
3 |
0 |
0 |
0 |
1 |
1 |
0 |
0 |
722 |
| Terveisiä huippuyliopistoista | 10 |
2 |
1 |
0 |
5 |
0 |
0 |
1 |
2 |
1 |
0 |
0 |
22 |
| Terveisiä huippuyliopistoista | 5 |
3 |
1 |
1 |
6 |
1 |
0 |
0 |
1 |
1 |
0 |
1 |
20 |
| The CMS Magnetic Field Map Performance | 6 |
2 |
2 |
2 |
3 |
4 |
0 |
0 |
1 |
0 |
0 |
0 |
20 |
| The CMS Magnetic Field Map Performance | 4 |
3 |
2 |
5 |
3 |
2 |
0 |
0 |
2 |
1 |
1 |
0 |
23 |
| The extraordinarily popular fixation with economic growth | 2 |
3 |
4 |
3 |
3 |
1 |
2 |
0 |
1 |
0 |
0 |
1 |
20 |
| The physics of spectral invariants | 8 |
3 |
2 |
2 |
3 |
2 |
1 |
0 |
2 |
0 |
0 |
0 |
23 |
| The physics of spectral invariants | 13 |
1 |
3 |
3 |
4 |
7 |
0 |
4 |
19 |
53 |
2 |
2 |
111 |
| Trust challenges for business-to-business networks | 2 |
3 |
1 |
1 |
5 |
1 |
0 |
0 |
0 |
0 |
1 |
0 |
14 |
| University of Helsinki Department of Computer Science Annual Report 1998 | 3 |
2 |
6 |
2 |
3 |
1 |
0 |
1 |
0 |
0 |
0 |
3 |
21 |
| Using IRAP markers for analysis of genetic variability in populations of resource and rare species of plants | 17 |
11 |
9 |
7 |
9 |
5 |
1 |
1 |
2 |
3 |
1 |
5 |
71 |
| Vibrational spectroscopy of trans and cis deuterated formic acid (HCOOD): Anharmonic calculations and experiments in argon and neon matrices | 7 |
4 |
4 |
1 |
5 |
4 |
0 |
0 |
3 |
2 |
0 |
4 |
34 |
| Yhteistoiminnallinen työskentely ja poikkitieteellisen asiantuntijuuden kehittyminen | 5 |
2 |
0 |
4 |
3 |
4 |
0 |
0 |
4 |
2 |
5 |
2 |
31 |