of fact, the NMP and MU labor demand elasticity coincide when β = 0 and the latter is
larger than the former when β → ∞. Thus it is sufficient to analyze if the slope of ⅛β1
evaluated at β = 0 is greater than ^βz- evaluated at β = 0. The impact of CBC on money
supply elasticity in both regimes at β = 0 is
dηu (1 — α)(1 — (1 — α)σ)
dβ J β=o k(n — 1)
and
dη n Θh [k + βp0“p — (kθh + βp@f(1 — α))σ]
dβ _ β=o k(n — 1)(k + βf@F)
(54)
(55)
Note, first, that expression (55) is an increasing function of βF. When σ > ɪɪ the ratio
№] β=o.βr =o
Γ ⅛. 1
( dβ β=o
1 — α7 — (1 — α7 )2σ
1 — a — (1 — α)2σ
(56)
which implies that there not exists a level of β = 0 where the labor demand elasticity
7∕n and ηu are equal. When σ < ɪɪ the expression (56) holds iff σ < 1-a^1-a^. ɪn such
a case there exists a level of β = 0 where the labor demand elasticity ηw and ηu intersect.
The second part of Proposition 5 is achieved by evaluating equation (50) at nH = 1 and
∏H → ∞. ■
Analysis of CSW and macroeconomic outcome. The marginal impact on labor
elasticity of a more decentralized wage setting is
dηw [(k^N + βF^F(1 — α))σ — (k + βfdF)] Z2
dnH ^ [к(пн — 1)(k + βFθF)+ пнβ(βFΘnΘf(1 — a) + k¾)]2
where Z2 ≡ β^N [k2 + βfβ^N@F(1 — a) + k(βfdF + β^N)] > 0 and the sign of ηN de-
pends on the
k k+ βf^F ʌ
"5n V — kθN + βFΘf (1 — a) )
By the same token, the derivative of the labor demand elasticity with respect to unions
numerosity is
dηu = ( —1 + Mu) [1 — (1 — oPσ]
dn [n + a(—1 + μu) — Mu]2
and the sign is determined by the
which proves Proposition 7. bterestingly, both labor elasticity tends to σ in presence of
atomistic wage setting (i.e. ∏h → ∞). ɪn order to compare the effect of CWS in the two
sign
(σ
33
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