150
Z. Xiang / Journal of Molecular Structure 1049 (2013) 149–156
(a)
COO-
R1
COOH
R1
R1
ESI(-)
R2
-CO2
R2-CHO
H2O
R2
N
R1
R2
R2
N
N
H2N
COOH
(b)
H2N
-CO2
R2
N
ESI(-)
COOH
R2-CHO
H2O
R2
N
COO-
N
n
n
n
COOH
n
R2= aryl; n=1, 2, 4
R1=-CH3, PhCH2-;
Scheme 1. Decarboxylation of the
a
-amino acid and non-a-amino acid anions catalyzed by the aromatic aldehyde.
Certain progress has been made in the carbonyl-catalyzed
ture: ꢁ240 °C; Sheath gas flow rate: 9.28 L/min; Tube lens: 55 V.
In the MS/MS experiments, the carboxylate anions have been
isolated monoisotopically in the ion trap and collisionally activated
by the same collision energies. Helium (99.99%) was used as the
trapping and collision gas.
decarboxylation of amino acids, however, to the best of our knowl-
edge, most of the investigations concentrate in the liquid reactions.
The rate of the decarboxylation is determined by the catalyst and
pH value of the solution. However, the carbonyl-catalyzed
decarboxylation of amino acids in the gas phase has received
considerably less attention. This makes us decide to explore the
gas-phase decarboxylation reactions of the amino acids with the
assistance of aromatic aldehyde from both experimental and com-
2.3. Computational methods
All structures were computed on the basis of the hybrid density
functional theory (M06-2X) [22] and the 6-31+G(d, p) basis set
which were implemented in Gaussian 09 program package [23].
All the gas phase minima and transition structures (here also re-
ferred to as transition states) were characterized by frequency
analysis. Frequency calculations identify minimum structures with
all real frequencies, while transition states with only one imagi-
nary frequency. Zero point energy (ZPE) corrections were applied
at the same level [24]. To confirm the transition states connecting
the designated intermediates, intrinsic reaction coordinate (IRC)
calculations were carried out. Furthermore, to obtain more reliable
energetic data, higher-level single-point energy calculations were
performed at M06-2X/6-311++G(3df, 2p) level by using the
M06-2X/6-31+G(d, p) optimized geometries.
putational perspective, as is shown in Scheme 1.
such as -alanine -phenylalanine and etc, and non-
such as b-alanine, -aminobutyric acid and -aminocaproic acid,
a
-Amino acids,
L
L
a-amino acids,
c
e
have been selected as the object of study. Herein, two items should
be emphasized. First, as this work focuses on the gas-phase decar-
boxylation of amino acid anion via imine intermediate, only aro-
matic aldehyde has been selected as the catalyst. The reason is
that the use of aliphatic aldehyde probably leads to the problem
of obtaining additional intermediates (enamines) which would
complicate the mechanistic study of the reactions involved. Sec-
ondly, the tandem mass spectrometry in the negative ion mode
has been used to study the decarboxylation of the amino acid
anion.
It is well known that the C@N bond widely exists in the
organocatalyses [19–21], because the formation of the C@N bond
can effectively increase the electrophilicity of the corresponding
carbonyl. In this paper, the influence that the C@N bond and ben-
zene ring exert on the dissociation of the CAC bond adjacent to the
carboxylate and the nature of the decarboxylation will be explored
by tandem mass spectrometry technique and DFT calculations.
3. Results and discussion
Several typical amino acids have been selected as the objects of
the investigation. Thereinto,
sent -amino acids, while non-
-aminobutyric acid and -aminocaproic acid. The examination
L
-alanine and
L-phenylalanine repre-
a
a-amino acids contain b-alanine,
c
e
of the direct decarboxylation of these amino acid anions without
any catalyst has been performed first. The deprotonated amino
acids can be prepared by electrospray ionization of a 3:1 (v/v)
acetonitrile/water solution containing these amino acids in the
negative ion mode. Then the collision-induced dissociation (CID)
experiments of these carboxylate anions will provide the informa-
tion on the decarboxylation in the gas phase. It is found that the
direct decarboxylation of these amino acid anions is hard to take
place. In order to avoid the case that the collision energy is not suf-
ficient to strike the CAC bond to lose CO2, collision energy scanning
within the range of possibilities has been performed; however, the
fragment ion due to the loss of CO2 has never been found. As the
decarboxylation of the carboxylate belongs to SE1 reaction [25–
27] (see Eqs. (1) and (2)), the rate-determining step is the dissoci-
ation of the adjacent CAC bond, which leads to the carbanion and
CO2. Thus, it is difficult for amino acid anion to lose CO2, maybe
because the producing carbanion is very unstable.
2. Experimental
2.1. Material
L
-alanine,
-aminocaproic acid, benzaldehyde, cinnamaldehyde, 4-methoxy-
benzaldehyde and 4-(dimethylamino)-benzaldehyde were
L-phenylalanine, b-alanine, c-aminobutyric acid,
e
obtained from the Sigma-Aldrich Company. These chemical
reagents with >95% purity have been used without further
purification.
2.2. Mass spectrometry
The mass spectral data were acquired on a LCQ ion trap mass
spectrometer from ThermoFinnigan (San Jose, CA, USA) equipped
with an electrospray ionization (ESI) interface operated in the
negative ion mode. ESI of a CH3CN/H2O (3:1) solution containing
amino acid (about 500
hyde was carried out at a flow rate of 15
R—X s!low Rꢂ þ Xþ
ð1Þ
ð2Þ
l
M) and a stoichiometric amount of alde-
SE1
l
L/min into the ESI
source. The operation parameters are listed as follows: spray tip
potential ꢁ3000 V; capillary voltage: ꢁ20 V; capillary tempera-
fast
R
ꢂ þ Yþ ! R—Y