Microscopi Elettronici a Scansione (SEM)

La Tescan è in grado di proporre una gamma completa di microscopi elettronici a scansione ad altissime performance, sia con sorgente termoionica che con sorgente a emissione di campo.

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SEM VEGA Compact

Microscopi SEM Termoionici

Il nuovo microscopio TESCAN VEGA Compact nasce dalla pluridecennale e consolidata esperienza della serie VEGA. La sua configurazione tecnica semplice e dal design molto compatto lo rende la scelta ideale per laboratori ed applicazioni dove è prioritaria una caratterizzazione di base dei campioni da analizzare.

Il SEM VEGA Compact è dotato di un innovativo design dell’elettrottica che consente un’immediata e semplicissima selezione delle condizioni di imaging o analitiche senza alcuna necessità di riallineamenti meccanici manuali in colonna.

Le caratteristiche principali della serie Vega Compact sono:

  • Tipologia emettitore: Termoionico
  • Risoluzioni: 3 nm @ 30 KeV e 8 nm @ 3 kV
  • Rivelatori standard: ET-SE e BSE
  • Corrente di sonda: da 1 pA a 2 µA
  • Ingrandimenti: da 2 X a 1.000.000 X
  • Tavolino portacampioni motorizzato su 5 assi
  • Dimensioni interne della camera (diametro): 230 mm
  • Software di Gestione EssenceTM con 3D Collision Model
  • EDX totalmente integrata con software EssenceTM

Per richiedere informazioni e brochures o per contattare lo specialista di prodotto compila il seguente form

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

SEM VEGA

Microscopi SEM Termoionici

Il nuovo microscopio TESCAN VEGA, giunto alla sua quarta generazione, nasce dalla pluridecennale e consolidata esperienza della serie VEGA. La sua configurazione tecnica lo rende la scelta ideale per la caratterizzazione di una grandissima varietà di campioni ed applicazioni.

Il nuovo TESCAN VEGA è dotato di un innovativo design dell’elettrottica che consente un’immediata e semplicissima selezione delle condizioni di imaging o analitiche  senza alcuna necessità di riallineamenti meccanici manuali in colonna.

Le caratteristiche principali della serie Vega sono:

  • Tipologia emettitore: Termoionico
  • Risoluzioni: 3 nm @ 30 KeV e 8 nm @ 3 kV
  • Rivelatori standard: ET-SE e BSE
  • Innovativa modalità SingleVacTM per compioni non conduttivi
  • Modalità HV ed LV (opzionale) fino a 500 Pa
  • Corrente di sonda: da 1 pA a 2 µA
  • Ingrandimenti: da 2 X a 1.000.000 X
  • Tavolino portacampioni motorizzato su 5 assi
  • Camere disponibili: di medie dimensioni (LM) o di grandi dimensioni (GM)
  • Software di Gestione EssenceTM con 3D Collision Model
  • EDX totalmente integrata con software EssenceTM

Per richiedere informazioni e brochures o per contattare lo specialista di prodotto compila il seguente form

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

FE-SEM MIRA

Microscopi ad Emissione di Campo FE-SEM

Il microscopio elettronico a scansione a emissione di campo TESCAN MIRA FE-SEM di quarta generazione è caratterizzato da un’esclusiva architettura della colonna elettronica a tre lenti che consente un’operatività estremamente semplificata rispetto al segmento tecnologico di riferimento.

Tale semplicità ed immediatezza di utilizzo lo rendono uno strumento particolarmente adatto per la caratterizzazione di un’ampia gamma di materiali in laboratori sia di analisi qualità che di ricerca e sviluppo.

Le caratteristiche principali della serie Mira sono:

  • Tipologia emettitore: di tipo Schottky termoassistita
  • Risoluzioni: 1 nm @ 30 KeV – 1,2 nm @ 15kV – 3,5 nm @ 1 kV
  • Rivelatori standard: ET-SE e BSE
  • Innovativa modalità SingleVacTM per compioni non conduttivi
  • Modalità HV ed LV (opzionale) fino a 500 Pa
  • Corrente di sonda: da 2 pA a 400 nA
  • Tavolino portacampioni motorizzato su 5 assi
  • Camere disponibili: di medie dimensioni (LM) o di grandi dimensioni (GM)
  • Ingrandimenti: da 1 X a 1.000.000 X con camera GM
  • Software di Gestione EssenceTM con 3D Collision Model
  • EDX totalmente integrata con software EssenceTM

Per richiedere informazioni e brochures o per contattare lo specialista di prodotto compila il seguente form

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

UHR FE-SEM CLARA

Microscopi ad Emissione di Campo FE-SEM di Classe UHR

Il nuovissimo UHR FE-SEM TESCAN CLARA è un microscopio elettronico a scansione ad ultra-alta risoluzione progettato per garantire elevatissime performance di imaging e di analisi sui più diversi campioni nelle più diverse condizioni operative.  Il SEM è dotato dell’innovativa tecnologia BrightBeamTM che combina una lente obiettivo elettrostatica/elettromagnetica con un sistema di rivelazione di nuova concezione. Il design della lente permette di lavorare ad altissima risoluzione anche alle bassissime tensioni di accelerazione (fino a 50eV). In aggiunta, il nuovo sistema di rivelatori permette la selezione dei segnali raccolti secondo il loro angolo di take off o la loro energia, garantendo in questo modo la raccolta di nuove informazioni sulla topografia e sulla natura chimica del campione.

Il FE-SEM CLARA è uno strumento altamente versatile, ideale per la caratterizzazione dei nanomateriali, per rigorosi controlli qualitativi su prodotti ed elevato contenuto tecnologico e per l’industria dei semiconduttori.

Le caratteristiche principali della serie Clara sono:

  • Tipologia emettitore: di tipo Schottky termoassistita
  • Risoluzione: 0,9 nm @ 15kV – 1,4 nm @ 1 kV
  • Rivelatori standard: ET-SE, BSE, Multidetector, Axial Detector
  • Modalità HV ed LV (opzionale) fino a 500 Pa
  • Corrente di sonda: da 2 pA a 400 nA
  • Tavolino portacampioni motorizzato su 5 assi
  • Camere disponibili: di medie dimensioni (LM) o di grandi dimensioni (GM)
  • Ingrandimenti: da 1 X a 1.000.000 X con camera GM
  • Software di Gestione EssenceTM con 3D Collision Model
  • Decontaminatore al Plasma integrato

Per richiedere informazioni e brochures o per contattare lo specialista di prodotto compila il seguente form

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

UHR FE-SEM MAGNA

Microscopi ad Emissione di Campo FE-SEM di Classe UHR

Il microscopio elettronico TESCAN MAGNA UHR FE-SEM rappresenta il sistema ideale di caratterizzazione superficiale di nanomateriali in particolare alle basse e bassissime tensioni di accelerazione ed in modalità STEM.

Il microscopio TESCAN MAGNA eccelle quindi nella caratterizzazione di materiali catalizzatori, nanotubi, nanoparticelle e strutture prefabbricate con dimensioni nanometriche quali i circuiti integrati di ultima generazione.

Le caratteristiche principali della serie Magna sono:

  • Tipologia emettitore: di tipo Schottky termoassistita
  • Risoluzione: 0,6 nm @ 15kV – 1,2 nm @ 1 kV
  • Rivelatori standard: ET-SE, BSE, Multidetector, Axial Detector
  • Modalità HV ed LV (opzionale) fino a 500 Pa
  • Corrente di sonda: da 2 pA a 400 nA
  • Tavolino portacampioni motorizzato su 5 assi
  • Camere disponibili: di medie dimensioni (LM) o di grandi dimensioni (GM)
  • Ingrandimenti: da 1 X a 1.000.000 X con camera GM
  • Software di Gestione EssenceTM con 3D Collision Model
  • Decontaminatore al Plasma integrato

Per richiedere informazioni e brochures o per contattare lo specialista di prodotto compila il seguente form

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

UHR FE-SEM FIB AMBER X

Sistemi UHR FE-SEM FIB con Colonna Ionica al Plasma di Xenon

Il nuovo UHR FE-SEM FIB TESCAN AMBER X è un Plasma FIB analitico ad Ultra Alta Risoluzione UHR.

Pensato per la caratterizzazione di campioni e materiali difficilmente gestibili con una colonna ionica al Ga, il sistema combina la colonna elettronica BrightBeamTM, che garantisce elevata risoluzione produttività, alla colonna ionica iFIB+TM al gas di Xenon. Il Plasma a ioni di Xenon consente di rimuovere elevate quantità di materiale e, data la natura inerte del gas, di ottenere preparazioni di campioni esenti da contaminazioni di Ga.

Le caratteristiche principali della serie AMBER X sono:

  • Colonna elettronica TESCAN BrightBeamTM Field-Free UHR-SEM
  • Tipologia emettitore: di tipo Schottky termoassistita
  • Risoluzione: 0,9 nm @ 15kV – 1,5 nm @ 1 kV
  • Corrente di sonda: da 2 pA a 400 nA
  • Rivelatori standard: ET-SE, BSE, Multidetector, Axial Detector
  • Colonna Ionica iFIB+TM al gas di Xenon
  • Risoluzione: <15 nm @ 30kV
  • Tavolino portacampioni motorizzato su 5 assi
  • Ingrandimenti: da 1 X a 1.000.000 X
  • Software di Gestione EssenceTM con 3D Collision Model
  • Decontaminatore al Plasma integrato

Per richiedere informazioni e brochures o per contattare lo specialista di prodotto compila il seguente form

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UHR FE-SEM FIB AMBER

Sistemi UHR FE-SEM FIB con Colonna Ionica al Gallio

Il nuovo UHR FE-SEM FIB TESCAN AMBER è stato progettato per l’ottenimento di una grande flessibilità e versatilità d’utilizzo.

La sinergia tra la sua colonna elettronica BrightBeamTM e la colonna ionica OrageTM al Ga, allo stato dell’arte, lo rendono una soluzione ideale sia per la caratterizzazione avanzata dei materiali sia per applicazioni di preparazione campioni nella scala micro/nanometrica.

Le caratteristiche principali della serie AMBER sono:

  • Colonna elettronica BrightBeamTM Field-Free UHR-SEM
  • Tipologia emettitore: di tipo Schottky termoassistita
  • Risoluzione: 0,9 nm @ 15kV – 1,5 nm @ 1 kV
  • Corrente di sonda: da 2 pA a 400 nA
  • Rivelatori standard: ET-SE, BSE, Multidetector, Axial Detector
  • Colonna Ionica OrageTM con sorgente LMIS
  • Risoluzione: 2,5 nm @ 30kV
  • Tavolino portacampioni motorizzato su 5 assi
  • Ingrandimenti: da 1 X a 1.000.000 X
  • Software di Gestione EssenceTM con 3D Collision Model
  • Decontaminatore al Plasma integrato

Per richiedere informazioni e brochures o per contattare lo specialista di prodotto compila il seguente form

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

UHR FE-SEM FIB SOLARIS

Sistemi UHR FE-SEM FIB con Colonna Ionica al Gallio

Il nuovo UHR FE-SEM FIB TESCAN SOLARIS rappresenta la piattaforma di lavoro ideale per applicazioni di nanofabbricazione avanzata.

Il sistema infatti utilizza sia la colonna ionica OrageTM al Ga, la più precisa e ad alta risoluzione attualmente disponibile, sia la colonna elettronica TriglavTM di ultra alta risoluzione.

Le caratteristiche tecniche di queste due colonne permettono il raggiungimento delle più elevate risoluzioni possibili richieste nei processi di prototipazione di dispositivi nanometrici e la fabbricazione di lamelle TEM di spessori estremamente sottili, fino a 10nm.

Le caratteristiche principali della serie SOLARIS sono:

  • Colonna elettronica TriglavTM UHR-SEM
  • Tipologia emettitore: di tipo Schottky termoassistita
  • Risoluzione: 0,6 nm @ 15kV – 1,2 nm @ 1 kV
  • Corrente di sonda: da 2 pA a 400 nA
  • Rivelatori standard: ET-SE, BSE, Multidetector, Axial Detector
  • Colonna Ionica OrageTM con sorgente LMIS
  • Risoluzione: 2,5 nm @ 30kV
  • Tavolino portacampioni motorizzato su 5 assi
  • Ingrandimenti: da 1 X a 1.000.000 X
  • Software di Gestione EssenceTM con 3D Collision Model
  • Decontaminatore al Plasma integrato

Per richiedere informazioni e brochures o per contattare lo specialista di prodotto compila il seguente form

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

UHR FE-SEM FIB SOLARIS X

Sistemi UHR FE-SEM FIB con Colonna Ionica al Plasma di Xenon

Il nuovo UHR FE-SEM FIB TESCAN SOLARIS X è la soluzione tecnologica ideale per la realizzazioni di sezioni ampie e profonde e per applicazioni avanzate di end-pointing per l’analisi dei fallimenti delle strutture di packaging di dispositivi a semiconduttore sia di tipo micromeccanico che optoelettronico.

La colonna al plasma di Xe consente di esporre superfici perfettamente lucide e prive di contaminazioni al Gallio e senza alcun tipo di danneggiamento meccanico indotto, come invece possibile con l’utilizzo di tecniche tradizionali di lucidatura.

Le caratteristiche principali della serie SOLARIS sono:

  • Colonna elettronica TriglavTM UHR-SEM
  • Tipologia emettitore: di tipo Schottky termoassistita
  • Risoluzione: 0,6 nm @ 15kV – 1,2 nm @ 1 kV
  • Corrente di sonda: da 2 pA a 400 nA
  • Rivelatori standard: ET-SE, BSE, Multidetector, Axial Detector
  • Colonna Ionica iFIB+TM al gas di Xenon
  • Risoluzione: <15 nm @ 30kV
  • Tavolino portacampioni motorizzato su 5 assi
  • Ingrandimenti: da 1 X a 1.000.000 X
  • Software di Gestione EssenceTM con 3D Collision Model
  • Decontaminatore al Plasma integrato

Per richiedere informazioni e brochures o per contattare lo specialista di prodotto compila il seguente form

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