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Lesson 15 The Transuranium Elements

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Lesson 15. The Transuranium Elements. The Basics. 118 known elements, 1- 118 All elements beyond 92 man-made. Modern Periodic Table. New element names/symbols 114=Fl= Flerovium 116= Lv = Livermorium. The history of the periodic table. The periodic table, circa 1940. - PowerPoint PPT Presentation

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Page 1: Lesson  15

Lesson 15

The Transuranium Elements

Page 2: Lesson  15

The Basics• 118 known elements, 1-118• All elements beyond 92 man-made

Page 3: Lesson  15

Modern Periodic Table

New element names/symbols 114=Fl=Flerovium116=Lv=Livermorium

Page 4: Lesson  15

The history of the periodic table

Page 5: Lesson  15

The periodic table, circa 1940

Page 6: Lesson  15

Making new elements by simple reactions

• The first man-made transuranium element, neptunium, Z=93

Page 7: Lesson  15

Making new elements by simple reactions (cont.)

• The second man-made transuranium element, plutonium, Z=94

The announcement of the discovery of Pu

Page 8: Lesson  15

Making new elements by simple reactions—the role of chemistry

• The discovery of elements 95(Am) and 96 (Cm)

Page 9: Lesson  15

Making new elements with nuclear weapons

• The synthesis of elements 99 (Md) and 100 (Fm)

Page 10: Lesson  15

MIKE

Samples of the bomb debris were collected on filter papers by aircraft flying through the mushroom cloud

Page 11: Lesson  15

Using heavy ion reactions to make new elements—The

Berkeley era

Albert Ghiorso Glenn Seaborg

Page 12: Lesson  15

Synthesis of elements 101-106

• Making elements one atom at a time• 254Es + 4He256Md + n

Page 13: Lesson  15

The problem

Page 14: Lesson  15

The Solution—The Darmstadt Era• “Cold Fusion” Reactions• Bombard Pb or Bi with heavy ions—

the resulting species are borne “cold” –with low excitation energies—they survive better

Peter Armbruster Sigurd HofmannYuri OganessianGottfried Munzenberg

Page 15: Lesson  15

The end of the “cold fusion” path

Page 16: Lesson  15

“Hot fusion-The Dubna Era”

Yuri Oganessian

Page 17: Lesson  15

History of Heavy Element Discoveries

• G.T. Seaborg and W. Loveland, The Elements Beyond Uranium

• S. Hofmann, On Beyond Uranium

• The textbook

Page 18: Lesson  15

The limits of the periodic table

• Can this go on forever? NO!!• Nature puts a limit on the size of

the periodic table, related to the relative strength of the electromagnetic and nuclear forces.

• The limit is about 125 elements.

Page 19: Lesson  15

The End of Chemistry• Does the Periodic Table have

limits? YES!!• At some point (Z~122) all the

electron energy levels of adjacent elements are similar so that there are no differences in their chemical behaviour.

Page 20: Lesson  15

Superheavy elements

Page 21: Lesson  15

Why are the “inert” gases inert?

• They have full shells of electrons• Full electron shells stability• Important exception: A professor

at UBC discovered many years ago that Xe could form chemical compounds with the very reactive element F.

Page 22: Lesson  15

Are there nuclei with special stability?

• Nuclei with full shells of neutrons and protons.

• Shell model of the nucleus• Special stability associated with

2,8,20, 28, 50,82, 126 neutrons or protons. (These are called the “magic numbers”)

• Where is the next proton magic number?

Page 23: Lesson  15

The “Island of Stability”

Page 24: Lesson  15
Page 25: Lesson  15

Superheavy elements

• The allegorical picture has stuck even though it is wrong. There is no “island of stability”

• “superheavy” = “shell-stabilized”

Page 26: Lesson  15

Current view

Page 27: Lesson  15

Methods of Heavy Element Synthesis

• Cold fusionPb, Bi as targetMassive ProjectileE*~ 13 MeV, high

survivalBig fusion hindranceUsed to synthesize

107-113

Page 28: Lesson  15

Methods of Heavy Element Synthesis

• Hot fusionReaction of lighter

projectile with actinide target

Low fusion hindrance

High E* (30-50 MeV), low survival

Used to synthesize 102-106, 113-118

Page 29: Lesson  15

How do you make heavy nuclei?

• Starting material• The latest synthesis of a chemical

element was the synthesis of element 117 via the reaction 249Bk(48Ca, 3n)294117.

• The two-year experimental campaign began with a 250-day irradiation in HFIR, producing 22 milligrams of berkelium-249, which has a 320-day half-life. The irradiation was followed by 90 days of processing at REDC to separate and purify the berkelium. The Bk-249 target was prepared at Dimitrovgrad and then bombarded for 150 days at the Dubna facility.

Page 30: Lesson  15
Page 31: Lesson  15

How do you make heavy nuclei?

• Particle accelerators

• Intense particle beams are needed. Cross sections are ~picobarns, which means one makes 1 atom per week. Cross sections as low as 32 femtobarns have been studied (1 atom/year)

Page 32: Lesson  15

How do you make heavy nuclei?

• Separators

Page 33: Lesson  15
Page 34: Lesson  15
Page 35: Lesson  15

Production of Heavy Elements in Complete Fusion Reactions

• We need to know three spin-dependent quantities: (a) the capture cross section, (b) the fusion probability and (c) the survival probability, and their isospin dependence

where

Page 36: Lesson  15

How well can we describe observations?

Page 37: Lesson  15

Let’s look at this more carefully

Page 38: Lesson  15

Despite correctly predicting σEVR correctly, , the values of PCN (and Wsur )differ significantly

Page 39: Lesson  15

Conclusions• For the 50-150 “calibration” reactions, we

know capture cross sections within 50%• We know interaction barriers within 20%• For the heavy element synthesis

reactions, we know the capture cross sections within a factor of 2.

• The “coupled channels” calculations (such as Zagrebaev) do the best overall job of describing capture cross sections.

Page 40: Lesson  15

What about Wsur?• Well-established formalism for

calculations• Principal uncertainty is the values

of the fission barrier heights.• Best calculations for SHE show an

average discrepancy between data and theory to be 0.4 MeV, with largest error being 1.0 MeV.

Page 41: Lesson  15

Γn/Γf evaluated from Vandenbosch and Huizenga expression

)1/2

fB*CNE

1/2nB

*CNE1/2exp(2a

11/22ak

)nB*CN(E2/34A

)*CN(EfΓ

)*CN(EnΓ

2/1*fCN BE

k=9.8 MeV a=A/12 MeV-1

Bn, Bf from Möller et al., (ADNDT 39,213; 59, 185)

xi

i Eifn

nxnsur EPW

max

1 *,

*)(

Calculation of Wsur

Collective enhancement of the level densityDeformation dependence of the collective enhancementEnergy dependence of the collective enhancement

Page 42: Lesson  15

How well can we calculate Wsur?

• We took a group (~75 ) heavy element synthesis reactions where Z1Z2 < 1000 (ZCN =98-108) and compared the calculated and measured values of σEVR.

• The average ratio of (measured/calculated) cross sections was 6.5. We conclude that we know Wsur within a factor of 3.

Page 43: Lesson  15

What about PCN?• This is the most difficult quantity to

estimate or measure.• There are a limited number of

measurements of PCN.

Page 44: Lesson  15

Excitation Energy Dependence of PCN

)(

exp1)*,(

*int

*

0

JEEP

JEPB

CNCN

Zagrebaev and Greiner

Page 45: Lesson  15

PCN (E*)

Page 46: Lesson  15

PCN (fissility)

Page 47: Lesson  15

Hot fusion systematics

E*=35 MeV

48Ca + X

Page 48: Lesson  15

Hot fusion predictions• 249Bk(48Ca,3n)294117 σEVR=1 pb.• 249Bk(50Ti,4n)295119 σEVR=0.07 pb.• 248Cm(54Cr,4n)302120 σEVR=0.02 pb.• 244Pu(58Fe,4n)302120 σEVR=0.006 pb.• 238U(64Ni,3n)302120 σEVR=0.004 pb. Based upon MNMS masses

Page 49: Lesson  15

Chemistry of the Heaviest Elements

• Relativistic Effects important since electron velocities approach that of the speed of light.

• Must use Dirac equation rather than the Schrodinger equation.

• Already known in Au, etc.

Page 50: Lesson  15

Relativistic Effects in Atomic Physics and Chemistry

• In high Z atoms. speed of inner electrons approaches c, mass of electron increases. Radius of orbits contracts.

For Sg, =0.77, a/a0=0.64

This defines the “direct relativistic effect” , ie. contraction of s and p1/2 orbitals

Page 51: Lesson  15

Direct Relativistic Effect

Page 52: Lesson  15

“Indirect” Relativistic Effect

• Due to contraction of s and p1/2 orbitals, outer electrons are more effectively screened and outer p,d,f orbitals expand.

Page 53: Lesson  15

Spin-Orbit Splitting• Levels with > 0, are split into

and

Page 54: Lesson  15

Effect of This

Page 55: Lesson  15

The “new” Aufbau diagram

Page 56: Lesson  15

Au--and heavier elements• Contraction of 6s, expansion of 5p

orbitals reduces the energy difference between these orbitals to that of a photon of blue light-> Au absorbs blue light and appears yellow.

• Non-relativistic -> Au would be unable to absorb light

Page 57: Lesson  15
Page 58: Lesson  15

Chemistry Apparatus• Rapid chemistry• Both gas and

liquid systems• Chemistry

separate from production.

Page 59: Lesson  15

Chemistry Apparatus

Page 60: Lesson  15

Chemistry of Element 112

Page 61: Lesson  15

Chemistry of element 114

• 3 events observed at Dubna by PSI group, corresponding to 287114, 288114, and 289114 from 48Ca + 242,244Pu. (Eichler et al, Radiochimica Acta 98, 133 (2010)). Conclude that element 114 seems to behave like a very volatile metal, with very weak interaction with Au – even weaker than element 112. Most likely gaseous at ambient temperatures.

 

Page 62: Lesson  15

Chemistry of element 114

Page 63: Lesson  15

More prosaic, yet vexing chemistry, Rf-Hs• Rf

Page 64: Lesson  15

Db• Expts.

complicated and difficult

• Not well understood

Page 65: Lesson  15

Sg• “Normal”

behavior

Page 66: Lesson  15

Bh• “the chemistry

of bohrium is boring”

Page 67: Lesson  15

Hs• Chemistry at

the 1 pb level

Page 68: Lesson  15

Environmental chemistry of the

transuranium elements• Plutonium is the most important

element.• Present due to atmospheric

testing, satellite re-entry and nuclear power accidents

• Extremely low concentrations (~10-

18M)• Low levels in soil, sediments, etc.

Page 69: Lesson  15

Aqueous environmental chemistry of Pu

• Hydrolysis• Complexation, redox reactions,

colloid formation also important.

• Hydrolyic seriesAn4+>AnO2

2+> An3+> AnO2+

Page 70: Lesson  15

Complexation